Dr. E. G. Rini Post Doctoral Fellow Centre for Material Science & Engineering.

Size: px
Start display at page:

Download "Dr. E. G. Rini Post Doctoral Fellow Centre for Material Science & Engineering."

Transcription

1 Research work focuses on: Lattice dynamics of materials using Rigid Ion Model, Shell Model, Density Functional Theory (DFT) Synthesis, characterization and physical properties of nanomaterials. Dr. E. G. Rini Post Doctoral Fellow Centre for Material Science & Engineering. Lattice dynamics of PrMnO3 & NdMnO3. (Work collaborated with BARC, Mumbai). The lattice dynamical properties of PrMnO3 and NdMnO3 were studied using shell model and First Principle Density Functional Theory (DFT). The investigations include the computation of the vibrational modes, leading to the phonon dispersion curves, phonon density of states, Raman and infrared frequencies, specific heat and electronic structure calculation which includes band structure, electron density of states of PrMnO3 & NdMnO3. These studies aimed at providing an understanding of the microscopic aspects of the thermodynamic properties of these parent manganites of the colossal magnetoresistance materials. Study of cohesion & structural properties of RMnO3 perovskite (R= La, Pr, Nd, Tb, Dy, Ho, Er). (Work collaborated with Dr. Savas Kaya, Cumhuriyet University, Turkey) A study of the cohesion and structural properties of RMnO3 perovskite have been carried out by means of an interatomic potential, which consists of the long-range Coulomb interactions & short range overlap repulsive interactions. Structural properties include cohesive energy, molecular force constant, bulk modulus, Debye temperature

2 & Reststrahlen frequency. The variation of Madelung energy & structural properties with decreasing ionic radii of R 3+ along the series RMnO3 (R=La to Er) has been studied. It is noticed that the short-range overlap repulsion is less than 15% of the total cohesive energy. This feature is indicative of the fact that major contribution to the cohesion in RMnO3 (R= La, Pr, Nd, Tb, Dy, Ho, Er) perovskite materials is due to coulomb attraction. It is well known that these static properties of the materials originate from the interatomic interactions between their atoms. Therefore, theoretical studies of static properties are very important because these properties are directly calculated from interatomic potential. Static properties like bulk modulus, molecular force constant, Reststrahlen frequency provides information regarding the stability & hardness of the material. Debye temperature gives information about the highest temperature that can be achieved due to a single normal vibration & hence it is important. Effect of Silicon substitution in ZnO: First Principle Density Functional Study. Band structure calculation, Electronic Density of States and phonon frequencies have been calculated for pure and silicon substituted ZnO. Project Proposal: First Principle Studies & Synthesis, characterization, physical properties of multiferroics RFeO3(R=Bi, Ga, La, Nd) nanoparticles submitted to DST. Ongoing Research Projects: *Study of effect of substitution of Vanadium in TiO2 using

3 DFT. *Study of effect of substitution of Iron in CuO2 using DFT. *Study of effect of substitution of Nickel in CeO2 using DFT. These studies focus on how physical and optical properties are affected with substitution. Publications: A. Book Cohesive and Thermal Properties of Colossal Magnetoresistive La0.88 Sr0.12 MnO3. E. G. Rini, N.K. Gaur, Vilas Shelke, M.P. Verma & R.K. Singh, in Phonons in Condensed Materials eds. S. P. Sanyal and R. K. Singh, (Allied, New Delhi, 2004), p.352. B. International Journals Phonon dynamics of lanthanum manganite LaMnO3 using an interatomic shell model potential E. G. Rini, Mala N. Rao, S. L. Chaplot, N. K. Gaur, and R. K. Singh, Phys. Rev. B 75 (2007) Phonon dispersion curves of CsCN N. K. Gaur, Preeti Singh, E. G. Rini, Jyotsna Galgale and R.K. Singh, Pramana 63 (2004) 419. Specific heat of LaMnO3+ δ at 50 K T 160 K. E.G. Rini, N.K. Gaur, Vilas Shelke, J. Galgale, M.P. Verma & R.K. Singh. Journal of Superconductivity, 15 (2002) 583. Effect of lattice distortion on bandgap decrement due to vanadium substitution in TiO2 nanoparticles Nasima Khatun, E. G. Rini, Parasharam Shirage, Parasmani Rajput, S. N. Jha and Somaditya Sen, Journal Material Science and Semiconducting Processing 50 (2016) 7-13.

4 Structural distortion and bandgap increment in nanocrystalline wurtzite Si substituted ZnO. Tulika Srivastava, E.G.Rini, Ashutosh Joshi, Parasharam Shirage and Somaditya Sen, J. Nanosci. Nanotechnol.16 (2016) 1 4. Structural and Mechanical characterization of Si doped ZnO. Gaurav Bajpai, Mohd Nasir, E. G. Rini, Sunil Kumar, Parasharam Shirage, and Somaditya Sen, Accepted in J. Nanosci. Nanotechnol. (2016). C. Conference Proceedings Thermodynamic properties of the orthorhombic manganites, LaMnO3 and YMnO3 Mala N. Rao, E.G. Rini, Nupinderjeet Kaur, N.K. Gaur, R.K. Singh and S.L. Chaplot, Presented in International Conference on Advanced Materials held at Bangalore, 8-13 October Lattice dynamics of the orthorhombic manganites, LaMnO3 and YMnO3 Mala N. Rao, E.G. Rini, Nupinderjeet Kaur, S. L. Chaplot, N.K. Gaur and R. K. Singh, Presented at International Symposium on Materials Chemistry held at BARC, 4-8 December Thermodynamic Properties of Colossal Magnetoresistance La1-x Srx MnO3 (0 x 0.16 ) compound. E.G. Rini Presented in XVIII Madhya Pradesh Young Scientist Congress Specific Heat of LaMnO3+ δ at 50 K T 160 K. E.G. Rini, N.K. Gaur, Vilas Shelke, J. Galgale, M.P. Verma & R.K. Singh. Presented in International Conference on Superconductivity, CMR and Related Materials at Giens, France during June1-8, 2002.

5 Static Shear Elasticity of (KCN)x(NaCN)1-x System. mixed Jyotsna Galgale, E. G. Rini, R.K. Singh & N.K. Gaur, Solid State Phys. (India), 44 (2001) 67. Phonon Dynamics of orientationally Disordered mixed Crystals rubidium cyanide & bromide. N.K. Gaur, Jyotsna Galgale, E. G. Rini, M. Manke & R.K. Singh, Solid State Phys. (India), 44 (2001) 295. Static Shear Elasticity of Disordered mixed Crystals. Jyotsna Galgale, E. G. Rini, D.C. Gupta, R.K. Singh & N.K. Gaur, Solid State Phys. (India), 43 (2000), pp

The Effect of Potassium Doping on Specific Heat of Rare Earth Manganite RMnO 3 (R=La, Pr).

The Effect of Potassium Doping on Specific Heat of Rare Earth Manganite RMnO 3 (R=La, Pr). The Effect of Potassium Doping on Specific Heat of Rare Earth Manganite RMnO 3 (R=La, Pr). Abstract Archana Srivastava * and N.K.Gaur 1 Department of Physics, Sri Sathya Sai College for Women, Bhopal 46224,

More information

Magnetization reversal and ferrimagnetism in Pr 1 x Nd x MnO 3

Magnetization reversal and ferrimagnetism in Pr 1 x Nd x MnO 3 Bull. Mater. Sci., Vol. 37, No. 4, June 2014, pp. 809 813. Indian Academy of Sciences. Magnetization reversal and ferrimagnetism in Pr 1 x Nd x MnO 3 SANJAY BISWAS, MOMIN HOSSAIN KHAN and SUDIPTA PAL*

More information

Assessment of Variation in Zero Field Hall Constant of Colossal Magnetoresistive Manganites (Re1-x AxMnO3)

Assessment of Variation in Zero Field Hall Constant of Colossal Magnetoresistive Manganites (Re1-x AxMnO3) ESSENCE - International Journal for Environmental Rehabilitation and Conservation Panwar & Kumar/VIII [2] 2017/103 107 Volume VIII [2] 2017 [103 107] [ISSN 0975-6272] [www.essence-journal.com] Assessment

More information

Transport and Magnetic Properties of La 0.85 Ca Mn 1-x Al x O 3 Manganites

Transport and Magnetic Properties of La 0.85 Ca Mn 1-x Al x O 3 Manganites Asian Journal of Chemistry Vol. 21, No. 1 (29), S86-9 Transport and Magnetic Properties of La.85 Ca. 15 Mn 1-x Al x O 3 Manganites G ANJUM and S MOLLAH Department of Physics, Aligarh Muslim University,

More information

INELASTIC NEUTRON SCATTERING AND LATTICE DYNAMICS OF NOVEL COMPOUNDS

INELASTIC NEUTRON SCATTERING AND LATTICE DYNAMICS OF NOVEL COMPOUNDS INELASTIC NEUTRON SCATTERING AND LATTICE DYNAMICS OF NOVEL COMPOUNDS R. Mittal and S. L. Chaplot Solid State Physics Division Bhabha Atomic Research Centre A b s t r a c t Using a combination of lattice

More information

Personal Data. Educational Qualification BIODATA

Personal Data. Educational Qualification BIODATA BIODATA Personal Data Name :- Dr. Bipul Rakshit Father s Name :- Biswanath Rakshit Age :- 34 Sex :- Male Date of birth :- 08 th January 1982 Marital status :- Single Nationality :- Indian Address for Department

More information

Higher Order Elastic Constants of Thorium Monochalcogenides

Higher Order Elastic Constants of Thorium Monochalcogenides Bulg. J. Phys. 37 (2010) 115 122 Higher Order Elastic Constants of Thorium Monochalcogenides K.M. Raju Department of Physics, Brahmanand P.G. College, Rath (Hamirpur), Uttar Pradesh, 210 431, India Received

More information

We are IntechOpen, the world s leading publisher of Open Access books Built by scientists, for scientists. International authors and editors

We are IntechOpen, the world s leading publisher of Open Access books Built by scientists, for scientists. International authors and editors We are IntechOpen, the world s leading publisher of Open Access books Built by scientists, for scientists 3,700 108,500 1.7 M Open access books available International authors and editors Downloads Our

More information

The electronic structure of materials 1

The electronic structure of materials 1 Quantum mechanics 2 - Lecture 9 December 18, 2013 1 An overview 2 Literature Contents 1 An overview 2 Literature Electronic ground state Ground state cohesive energy equilibrium crystal structure phase

More information

LEAD-CHALCOGENIDES UNDER PRESSURE: AB-INITIO STUDY

LEAD-CHALCOGENIDES UNDER PRESSURE: AB-INITIO STUDY International Conference on Ceramics, Bikaner, India International Journal of Modern Physics: Conference Series Vol. 22 (2013) 612 618 World Scientific Publishing Company DOI: 10.1142/S201019451301074X

More information

University of Groningen. Orbital ordering and multiferroics Nenert, Gwilherm

University of Groningen. Orbital ordering and multiferroics Nenert, Gwilherm University of Groningen Orbital ordering and multiferroics Nenert, Gwilherm IMPORTANT NOTE: You are advised to consult the publisher's version (publisher's PDF) if you wish to cite from it. Please check

More information

Doctor of Philosophy

Doctor of Philosophy FEMTOSECOND TIME-DOMAIN SPECTROSCOPY AND NONLINEAR OPTICAL PROPERTIES OF IRON-PNICTIDE SUPERCONDUCTORS AND NANOSYSTEMS A Thesis Submitted for the degree of Doctor of Philosophy IN THE FACULTY OF SCIENCE

More information

Terahertz Spectroscopy for Quantum Condensed Matter Dhanvir Singh Rana

Terahertz Spectroscopy for Quantum Condensed Matter Dhanvir Singh Rana Terahertz Spectroscopy for Quantum Condensed Matter Dhanvir Singh Rana Department of Physics Indian Institute of Science Education and Research (IISER) Bhopal Terahertz spectroscopy on complex oxide films

More information

Recent Developments in Magnetoelectrics Vaijayanti Palkar

Recent Developments in Magnetoelectrics Vaijayanti Palkar Recent Developments in Magnetoelectrics Vaijayanti Palkar Department of Condensed Matter Physics & Materials Science Tata Institute of Fundamental Research Mumbai 400 005, India. Tata Institute of Fundamental

More information

c Indian Academy of Sciences.

c Indian Academy of Sciences. Bull. Mater. Sci., Vol. 36, No. 7, December 213, pp. 1255 126. c Indian Academy of Sciences. Phonon, magnon and electron contributions to low temperature specific heat in metallic state of La 85 Sr 15

More information

Structural Study of [Nd 0.5 (Ca 0.25 Ba 0.25 ) MnO 3 ] and [Nd 0.5 (Ca 0.25 Sr 0.25 )MnO 3 ] Perovskites at Room Temperature

Structural Study of [Nd 0.5 (Ca 0.25 Ba 0.25 ) MnO 3 ] and [Nd 0.5 (Ca 0.25 Sr 0.25 )MnO 3 ] Perovskites at Room Temperature Egypt. J. Sol., Vol. (24), No. (1), (2001) 33 Structural Study of [Nd 0.5 (Ca 0.25 Ba 0.25 ) MnO 3 ] and [Nd 0.5 (Ca 0.25 Sr 0.25 )MnO 3 ] Perovskites at Room Temperature F. F. Hanna Faculty of Petroleum

More information

Negative thermal expansion in framework compounds

Negative thermal expansion in framework compounds PRAMANA c Indian Academy of Sciences Vol. 7, No. 4 journal of October 28 physics pp. 829 835 Negative thermal expansion in framework compounds R MITTAL Forschungszentrum Jülich GmbH, Jülich Centre for

More information

Phonon Dispersion, Interatomic Force Constants Thermodynamic Quantities

Phonon Dispersion, Interatomic Force Constants Thermodynamic Quantities Phonon Dispersion, Interatomic Force Constants Thermodynamic Quantities Umesh V. Waghmare Theoretical Sciences Unit J N C A S R Bangalore ICMR OUTLINE Vibrations and interatomic force constants (IFC) Extended

More information

Center for Materials Science and Engineering. Indian Institute of Technology Ind ore

Center for Materials Science and Engineering. Indian Institute of Technology Ind ore Center for Materials Science and Engineering Indian Institute of Technology Ind ore Materials Science & Engineering Inter - disciplinary Research Group, IIT Indore Academic Programs and Facilities Ph.D

More information

Lattice dynamics of ferromagnetic superconductor UGe 2

Lattice dynamics of ferromagnetic superconductor UGe 2 PRAMANA c Indian Academy of Sciences Vol. 71, No. 5 journal of November 2008 physics pp. 1147 1151 Lattice dynamics of ferromagnetic superconductor UGe 2 SATYAM SHINDE 1 and PRAFULLA K JHA 2, 1 Nirma University

More information

On Dynamic and Elastic Stability of Lanthanum Carbide

On Dynamic and Elastic Stability of Lanthanum Carbide Journal of Physics: Conference Series On Dynamic and Elastic Stability of Lanthanum Carbide To cite this article: B D Sahoo et al 212 J. Phys.: Conf. Ser. 377 1287 Recent citations - Theoretical prediction

More information

Raman spectroscopy of orthorhombic perovskitelike YMnO 3 and LaMnO 3

Raman spectroscopy of orthorhombic perovskitelike YMnO 3 and LaMnO 3 PHYSICAL REVIEW B VOLUME 57, NUMBER 5 1 FEBRUARY 1998-I Raman spectroscopy of orthorhombic perovskitelike YMnO 3 and LaMnO 3 M. N. Iliev M. V. Abrashev* Institut für Festkörperphysik, Technische Universität

More information

Ionic Bonding - Electrostatic Interactions and Polarization

Ionic Bonding - Electrostatic Interactions and Polarization Ionic Bonding - Electrostatic Interactions and Polarization Chemistry 754 Solid State Chemistry Dr. Patrick Woodward Lecture #13 Born-Haber Cycle for NaCl It is energetically unfavorable for Na metal and

More information

lectures accompanying the book: Solid State Physics: An Introduction, by Philip ofmann (2nd edition 2015, ISBN-10: 3527412824, ISBN-13: 978-3527412822, Wiley-VC Berlin. www.philiphofmann.net 1 Bonds between

More information

The broad topic of physical metallurgy provides a basis that links the structure of materials with their properties, focusing primarily on metals.

The broad topic of physical metallurgy provides a basis that links the structure of materials with their properties, focusing primarily on metals. Physical Metallurgy The broad topic of physical metallurgy provides a basis that links the structure of materials with their properties, focusing primarily on metals. Crystal Binding In our discussions

More information

Internal friction and Jahn-Teller effect in the charge-ordered

Internal friction and Jahn-Teller effect in the charge-ordered Internal friction and Jahn-Teller effect in the charge-ordered La 1-x Ca x MnO 3 (0.5 x 0.87) R. K. Zheng, R. X. Huang, A. N. Tang, G. Li, X. G. Li a) Structure Research Laboratory, Department of Materials

More information

Non linear properties of mixed divalent crystals

Non linear properties of mixed divalent crystals Non linear properties of mixed divalent crystals Virendra Kumar Department of physics, B.N.P.G. College, Rath, Hamirpur, U.P., 10 431, Bharat Email- vir.rath@yahoo.com PACS: 6.0Dc, 6.65+K, 81.40Ji. ABSTRACT

More information

Chapter 3. Crystal Binding

Chapter 3. Crystal Binding Chapter 3. Crystal Binding Energy of a crystal and crystal binding Cohesive energy of Molecular crystals Ionic crystals Metallic crystals Elasticity What causes matter to exist in three different forms?

More information

Structural stability of TiO and TiN under high pressure

Structural stability of TiO and TiN under high pressure Cent. Eur. J. Phys. 6(2) 2008 277-282 DOI: 10.2478/s11534-008-0027-z Central European Journal of Physics Structural stability of TiO and TiN under high pressure Research Article Raja Chauhan 1, Sadhna

More information

Theory of divalent ions in crystals

Theory of divalent ions in crystals Pramina, Vol. 21, No. 5, November 1983, pp. 301-309. Printed in India. Theory of divalent ions in crystals G RAGHURAMA and RAMESH NARAYAN* Department of Physics, Indian Institute of Science, Bangalore

More information

Ultrashort Lifetime Expansion for Resonant Inelastic X-ray Scattering. Luuk Ament

Ultrashort Lifetime Expansion for Resonant Inelastic X-ray Scattering. Luuk Ament Ultrashort Lifetime Expansion for Resonant Inelastic X-ray Scattering Luuk Ament In collaboration with Jeroen van den Brink and Fiona Forte What is RIXS? Resonant Inelastic X-ray Scattering Synchrotron

More information

NEW ROUTES TO MULTIFERROICS

NEW ROUTES TO MULTIFERROICS NEW ROUTES TO MULTIFERROICS C. N. R. RAO Jawaharlal Nehru Centre for Advanced Scientific Research & Indian Institute of Science Bangalore, India 1 MULTIFERROICS Ferromagnetic Ferroelectric Ferroelastic

More information

Electronic structure calculations results from LDA+U method

Electronic structure calculations results from LDA+U method Electronic structure calculations results from LDA+U method Vladimir I. Anisimov Institute of Metal Physics Ekaterinburg, Russia LDA+U method applications Mott insulators Polarons and stripes in cuprates

More information

Structure and Dynamics : An Atomic View of Materials

Structure and Dynamics : An Atomic View of Materials Structure and Dynamics : An Atomic View of Materials MARTIN T. DOVE Department ofearth Sciences University of Cambridge OXFORD UNIVERSITY PRESS Contents 1 Introduction 1 1.1 Observations 1 1.1.1 Microscopic

More information

Raman Studies on Functional Perovskite Oxides

Raman Studies on Functional Perovskite Oxides Raman Studies on Functional Perovskite Oxides Venkata S. Bhadram Postdoctoral Research Associate Geophysical Laboratory Carnegie Institution for Science Bangalore Jawaharlal Nehru Centre for Advanced Scientific

More information

Name and Address of the University: The University of Burdwan, Burdwan , West Bengal, India

Name and Address of the University: The University of Burdwan, Burdwan , West Bengal, India 1 Science Physics Prof. SarbeswarChoudhur y DATA REGARDING PH. SCHOLARS Department of Physics Name and Address of the University: The University of Burdwan, Burdwan - 713104, West Bengal, India. Supriya

More information

equation of state and bulk modulus of AlP, AlAs and AlSb semiconductor compounds

equation of state and bulk modulus of AlP, AlAs and AlSb semiconductor compounds PRAMANA c Indian Academy of Sciences Vol. 64, No. 1 journal of January 2005 physics pp. 153 158 Total energy, equation of state and bulk modulus of AlP, AlAs and AlSb semiconductors A R JIVANI, H J TRIVEDI,

More information

Neutron Scattering in Transition Metal Oxides

Neutron Scattering in Transition Metal Oxides Neutron Scattering in Transition Metal Oxides C. Ulrich Department Prof. B. Keimer Max-Planck-Institut für Festkörperforschung, Stuttgart, Germany physics of the 3d electrons strongly correlated electrons

More information

Foundations of Condensed Matter Physics

Foundations of Condensed Matter Physics Foundations of Condensed Matter Physics PHY1850F 2005 www.physics.utoronto.ca/~wei/phy1850f.html Physics 1850F Foundations of Condensed Matter Physics Webpage: www.physics.utoronto.ca/~wei/phy1850f.html

More information

ELEMENTARY BAND THEORY

ELEMENTARY BAND THEORY ELEMENTARY BAND THEORY PHYSICIST Solid state band Valence band, VB Conduction band, CB Fermi energy, E F Bloch orbital, delocalized n-doping p-doping Band gap, E g Direct band gap Indirect band gap Phonon

More information

Electronic and vibrational Raman spectroscopy of Nd 0.5 Sr 0.5 MnO 3 through the phase transitions

Electronic and vibrational Raman spectroscopy of Nd 0.5 Sr 0.5 MnO 3 through the phase transitions PRAMANA c Indian Academy of Sciences Vol. 64, No. 1 journal of January 2005 physics pp. 119 128 Electronic and vibrational Raman spectroscopy of Nd 0.5 Sr 0.5 MnO 3 through the phase transitions Md MOTIN

More information

Colossal magnetoresistance:

Colossal magnetoresistance: Colossal magnetoresistance: Ram Seshadri (seshadri@mrl.ucsb.edu) The simplest example of magnetoresistance is transverse magnetoresistance associated with the Hall effect: H + + + + + + + + + + E y - -

More information

REVIEW : INTRODUCTION TO THE MOLECULAR ORIGINS OF MECHANICAL PROPERTIES QUANTITATIVE TREATMENT OF INTERATOMIC BONDING : THE LENNARD-JONES POTENTIAL

REVIEW : INTRODUCTION TO THE MOLECULAR ORIGINS OF MECHANICAL PROPERTIES QUANTITATIVE TREATMENT OF INTERATOMIC BONDING : THE LENNARD-JONES POTENTIAL LECTURE #19 : 3.11 MECANICS OF MATERIALS F3 INSTRUCTOR : Professor Christine Ortiz OFFICE : 13-422 PONE : 452-384 WWW : http://web.mit.edu/cortiz/www REVIEW : INTRODUCTION TO TE MOLECULAR ORIGINS OF MECANICAL

More information

Metal-insulator transitions

Metal-insulator transitions Metal-insulator transitions Bandwidth control versus fillig control Strongly correlated Fermi liquids Spectral weight transfer and mass renormalization Bandwidth control Filling control Chemical potential

More information

Supporting Information

Supporting Information Supporting Information Splitting of CO 2 by Manganite Perovskites to Generate CO by Solar Isothermal Redox Cycling Sunita Dey and C. N. R. Rao* Chemistry and Physics of Materials Unit, Sheikh Saqr Laboratory,

More information

High T C copper oxide superconductors and CMR:

High T C copper oxide superconductors and CMR: High T C copper oxide superconductors and CMR: Ram Seshadri (seshadri@mrl.ucsb.edu) The Ruddlesden-Popper phases: Ruddlesden-Popper phases are intergrowths of perovskite slabs with rock salt slabs. First

More information

Material Science II. d Electron systems

Material Science II. d Electron systems Material Science II. d Electron systems 1. Electronic structure of transition-metal ions (May 23) 2. Crystal structure and band structure (June 13) 3. Mott s (June 20) 4. Metal- transition (June 27) 5.

More information

Lecture 6 - Bonding in Crystals

Lecture 6 - Bonding in Crystals Lecture 6 onding in Crystals inding in Crystals (Kittel Ch. 3) inding of atoms to form crystals A crystal is a repeated array of atoms Why do they form? What are characteristic bonding mechanisms? How

More information

Ferroelectricity, Magnetism, and Multiferroicity. Kishan K. Sinha Xu Lab Department of Physics and astronomy University of Nebraska-Lincoln

Ferroelectricity, Magnetism, and Multiferroicity. Kishan K. Sinha Xu Lab Department of Physics and astronomy University of Nebraska-Lincoln Ferroelectricity, Magnetism, and Multiferroicity Kishan K. Sinha Xu Lab Department of Physics and astronomy University of Nebraska-Lincoln Magnetism, Ferroelectricity, and Multiferroics Magnetism o Spontaneous

More information

Structural elastic and thermal properties of Sr x Cd 1 x O mixed compounds a theoretical approach

Structural elastic and thermal properties of Sr x Cd 1 x O mixed compounds a theoretical approach Materials Science-Poland, 32(3), 2014, pp. 350-357 http://www.materialsscience.pwr.wroc.pl/ DOI: 10.2478/s13536-013-0197-2 Structural elastic and thermal properties of Sr x Cd 1 x O mixed compounds a theoretical

More information

The effect of Coulomb correlation and magnetic ordering on the electronic structure of two hexagonal phases of ferroelectromagnetic YMnO 3

The effect of Coulomb correlation and magnetic ordering on the electronic structure of two hexagonal phases of ferroelectromagnetic YMnO 3 J. Phys.: Condens. Matter 1 () 4947 4958. Printed in the UK PII: S953-8984()1985- The effect of Coulomb correlation and magnetic ordering on the electronic structure of two hexagonal phases of ferroelectromagnetic

More information

Multiferroic properties of Mn doped La 0.8 Bi 0.2 FeO 3 system and effect of SHI irradiation

Multiferroic properties of Mn doped La 0.8 Bi 0.2 FeO 3 system and effect of SHI irradiation Multiferroic properties of Mn doped La 0.8 Bi 0.2 FeO 3 system and effect of SHI irradiation THESIS ABSTRACT SUBMITTED FOR THE AWARD OF THE DEGREE OF DOCTOR OF PHILOSOPHY IN PHYSICS BY GHAZALA ANJUM UNDER

More information

What so special about LaAlO3/SrTiO3 interface? Magnetism, Superconductivity and their coexistence at the interface

What so special about LaAlO3/SrTiO3 interface? Magnetism, Superconductivity and their coexistence at the interface What so special about LaAlO3/SrTiO3 interface? Magnetism, Superconductivity and their coexistence at the interface Pramod Verma Indian Institute of Science, Bangalore 560012 July 24, 2014 Pramod Verma

More information

Lattice Vibrations. Chris J. Pickard. ω (cm -1 ) 200 W L Γ X W K K W

Lattice Vibrations. Chris J. Pickard. ω (cm -1 ) 200 W L Γ X W K K W Lattice Vibrations Chris J. Pickard 500 400 300 ω (cm -1 ) 200 100 L K W X 0 W L Γ X W K The Breakdown of the Static Lattice Model The free electron model was refined by introducing a crystalline external

More information

A PSEUDOPOTENTIAL STUDY ON THE THERMODYNAMIC AND ELASTIC PROPERTIES OF Pd 39 Ni 10 Cu 30 P 21 BULK METALLIC GLASS

A PSEUDOPOTENTIAL STUDY ON THE THERMODYNAMIC AND ELASTIC PROPERTIES OF Pd 39 Ni 10 Cu 30 P 21 BULK METALLIC GLASS A PSEUDOPOTENTIAL STUDY ON THE THERMODYNAMIC AND ELASTIC PROPERTIES OF Pd 39 Ni 10 Cu 30 P 21 BULK METALLIC GLASS Alkesh L. Gandhi Asst. Prof., Department of Physics, B. V. Shah(Vadi-Vihar) Science College,

More information

New lithium-ion conducting perovskite oxides related to (Li, La)TiO 3

New lithium-ion conducting perovskite oxides related to (Li, La)TiO 3 Proc. Indian Acad. Sci. (Chem. Sci.), Vol. 113, Nos 5 & 6, October December 2001, pp 427 433 Indian Academy of Sciences New lithium-ion conducting perovskite oxides related to (Li, La)TiO 3 1. Introduction

More information

CHAPTER: 8. ELECTRONIC STRUCTURE AND ELASTIC PROPERTIES OF CrC AND CrN. 8.1 Introduction. Ph.D. Thesis: J. Maibam

CHAPTER: 8. ELECTRONIC STRUCTURE AND ELASTIC PROPERTIES OF CrC AND CrN. 8.1 Introduction. Ph.D. Thesis: J. Maibam CHAPTER -8 CHAPTER: 8 ELECTRONIC STRUCTURE AND ELASTIC PROPERTIES OF CrC AND CrN 8.1 Introduction In this chapter, we have selected CrC and CrN from group VIB transition metal carbides and nitrides for

More information

Relation Between Refractive Index, Micro Hardness and Bulk Modulus of A II B VI and A III B V Semiconductors

Relation Between Refractive Index, Micro Hardness and Bulk Modulus of A II B VI and A III B V Semiconductors International Journal of Pure and Applied Physics ISSN 0973-1776 Volume 5, Number 3 (2009), pp. 271-276 Research India Publications http://www.ripublication.com/ijpap.htm Relation Between Refractive Index,

More information

Journal Publications:

Journal Publications: DR NAVAJYOTI CHOUDHURY Associate Professor Department of Physics Pub Kamrup College Baihata Chariali Journal Publications: 1. P.K. Mochahari, Ananta Rajbongshi, N. Choudhury, F. Singh and K.C. Sarma, Study

More information

CHAPTER 3. OPTICAL STUDIES ON SnS NANOPARTICLES

CHAPTER 3. OPTICAL STUDIES ON SnS NANOPARTICLES 42 CHAPTER 3 OPTICAL STUDIES ON SnS NANOPARTICLES 3.1 INTRODUCTION In recent years, considerable interest has been shown on semiconducting nanostructures owing to their enhanced optical and electrical

More information

Magnetic Phase Diagrams of Manganites in the Electron Doping Region

Magnetic Phase Diagrams of Manganites in the Electron Doping Region Physics of the Solid State, Vol. 46, No., 4, pp. 93. Translated from Fizika Tverdogo Tela, Vol. 46, No., 4, pp. 93. Original Russian Text Copyright 4 by Dunaevskiœ. REVIEWS Magnetic Phase Diagrams of Manganites

More information

Intrinsic chemical and structural inhomogeneity in lightly doped La 1-x Sr x MnO 3

Intrinsic chemical and structural inhomogeneity in lightly doped La 1-x Sr x MnO 3 Intrinsic chemical and structural inhomogeneity in lightly doped La 1-x x MnO 3 Tomohiro Shibata, a Bruce Bunker, a John Mitchell, b and Peter Schiffer c a) Department of Physics, University of Notre Dame,

More information

Ultrafast X-ray Spectroscopy of Solvated Transition-metal Complexes and Oxide Materials

Ultrafast X-ray Spectroscopy of Solvated Transition-metal Complexes and Oxide Materials Ultrafast X-ray Spectroscopy of Solvated Transition-metal Complexes and Oxide Materials Robert Schoenlein Materials Sciences Division Chemical Sciences Division - UXSL Matteo Rini ils Huse F. Reboani &

More information

Physical and dielectric properties of Bi 4 x R x Sr 3 Ca 3 Cu 2 O 10 glasses (x = 0.5 and R = Ag, Ni)

Physical and dielectric properties of Bi 4 x R x Sr 3 Ca 3 Cu 2 O 10 glasses (x = 0.5 and R = Ag, Ni) JOURNAL OF MATERIALS SCIENCE 34 (1999)3853 3858 Physical and dielectric properties of Bi 4 x R x Sr 3 Ca 3 Cu 2 O 10 glasses (x = 0.5 and R = Ag, Ni) A. MEMON, D. B. TANNER Department of Physics, University

More information

E12 UNDERSTANDING CRYSTAL STRUCTURES

E12 UNDERSTANDING CRYSTAL STRUCTURES E1 UNDERSTANDING CRYSTAL STRUCTURES 1 Introduction In this experiment, the structures of many elements and compounds are rationalized using simple packing models. The pre-work revises and extends the material

More information

Lattice effects in La 1 x Ca x MnO 3 x 0 1 : Relationships between distortions, charge distribution, and magnetism

Lattice effects in La 1 x Ca x MnO 3 x 0 1 : Relationships between distortions, charge distribution, and magnetism PHYSICAL REVIEW B VOLUME 57, NUMBER 17 1 MAY 1998-I Lattice effects in La 1 x Ca x MnO 3 x 0 1 : Relationships between distortions, charge distribution, and magnetism C. H. Booth* Department of Physics

More information

Phonon dispersion relation of liquid metals

Phonon dispersion relation of liquid metals PRAMANA c Indian Academy of Sciences Vol. 7, No. 6 journal of June 9 physics pp. 145 149 Phonon dispersion relation of liquid metals P B THAKOR 1,, P N GAJJAR A R JANI 3 1 Department of Physics, Veer Narmad

More information

A simple model for calculating the bulk modulus of the mixed ionic crystal: NH 4 Cl 1 x Br x

A simple model for calculating the bulk modulus of the mixed ionic crystal: NH 4 Cl 1 x Br x PRAMANA c Indian Academy of Sciences Vol. 77, No. 4 journal of October 2011 physics pp. 689 695 A simple model for calculating the bulk modulus of the mixed ionic crystal: NH 4 Cl 1 x Br x VASSILIKI KATSIKA-TSIGOURAKOU

More information

Phonon properties of rare earth ytterbium pnictides

Phonon properties of rare earth ytterbium pnictides PRAMANA Printed in India Vol. 44, No. 5, journal of May 1995 physics pp. 419-427 PRAFULLA K JHA and SANKAR P SANYAL Department of Physics, C V Raman Building, University of Bhopal, Bhopal 462 26, India.

More information

Dr. TANVEER AHMAD DAR

Dr. TANVEER AHMAD DAR CURRICULUM VITAE Dr. TANVEER AHMAD DAR S/O: Mr. AB. JABAR DAR Department of Physics, Islamic University of Science and Technology Awantipora, Pulwama, J & K- 192122. Contact: +91-9522559461, +91-9419046187

More information

Challenges for Materials to Support Emerging Research Devices

Challenges for Materials to Support Emerging Research Devices Challenges for Materials to Support Emerging Research Devices C. Michael Garner*, James Hutchby +, George Bourianoff*, and Victor Zhirnov + *Intel Corporation Santa Clara, CA + Semiconductor Research Corporation

More information

Scientific opportunities with ultrafast electron diffraction & microscopy

Scientific opportunities with ultrafast electron diffraction & microscopy Scientific opportunities with ultrafast electron diffraction & microscopy Jim Cao Frontier of ultrafast science MeV UED Transition pathways Rate and time scale Elementary steps Probe dynamics on the atomic

More information

Solid State Spectroscopy Problem Set 7

Solid State Spectroscopy Problem Set 7 Solid State Spectroscopy Problem Set 7 Due date: June 29th, 2015 Problem 5.1 EXAFS Study of Mn/Fe substitution in Y(Mn 1-x Fe x ) 2 O 5 From article «EXAFS, XANES, and DFT study of the mixed-valence compound

More information

Solid State Physics (Major, 8 ECTS)

Solid State Physics (Major, 8 ECTS) Solid State Physics (Major, 8 ECTS) 1 physicist over 3 in US declares to be a condensed matter physicist (CMP) CMP: solids, amorphous materials, liquids, soft materials 20 CMP physics Nobel prizes + 5

More information

Monitoring the Aggregation of Particles through Raman Spectroscopy

Monitoring the Aggregation of Particles through Raman Spectroscopy Monitoring the Aggregation of Particles through Raman Spectroscopy Name: Yanxiao Ma Advisor: Dr. Andrew Callender Submission Date: 19 Oct. 2012 Introduction Raman spectroscopy is a spectroscopic technique

More information

Bound small hole polarons in oxides and related materials: strong colorations and high ionization energies

Bound small hole polarons in oxides and related materials: strong colorations and high ionization energies Bound small hole polarons in oxides and related materials: strong colorations and high ionization energies O. F. Schirmer Universität Osnabrück central example: acceptor Li + Zn in ZnO O O 2 Small polaron:

More information

Local Structure of Mn in (La 1 x Ho x ) 2/3 Ca 1/3 MnO 3 Studied by X-ray Absorption Fine Structure

Local Structure of Mn in (La 1 x Ho x ) 2/3 Ca 1/3 MnO 3 Studied by X-ray Absorption Fine Structure Vol. 117 (2010) ACTA PHYSICA POLONICA A No. 2 Proceedings of the KSUPS Local Structure of Mn in (La 1 x Ho x ) 2/3 Ca 1/3 MnO 3 Studied by X-ray Absorption Fine Structure A. Pietnoczka a,, M. Pękała b,

More information

On conduction mechanism in paramagnetic phase of Gd based manganites

On conduction mechanism in paramagnetic phase of Gd based manganites Bull. Mater. Sci., Vol. 35, No. 1, February 2012, pp. 41 45. c Indian Academy of Sciences. On conduction mechanism in paramagnetic phase of Gd based manganites S SAGAR 1,2 and M R ANANTHARAMAN 1, 1 Department

More information

Chapter 2. Methodology. 2.1 Introduction

Chapter 2. Methodology. 2.1 Introduction Chapter 2 2.1 Introduction Over the past twenty years, one of the major developments in the physical and biological sciences is the use of computer modelling. For example, impressive achievements have

More information

Canadian Journal of Physics. Higher Order derivatives of bulk modulus of materials at infinite pressure

Canadian Journal of Physics. Higher Order derivatives of bulk modulus of materials at infinite pressure Higher Order derivatives of bulk modulus of materials at infinite pressure Journal: Manuscript ID cjp-015-0699.r Manuscript Type: Article Date Submitted by the Author: 0-Apr-016 Complete List of Authors:

More information

Impact of size and temperature on thermal expansion of nanomaterials

Impact of size and temperature on thermal expansion of nanomaterials PRAMANA c Indian Academy of Sciences Vol. 84, No. 4 journal of April 205 physics pp. 609 69 Impact of size and temperature on thermal expansion of nanomaterials MADAN SINGH, and MAHIPAL SINGH 2 Department

More information

Magnetic Oxides. Gerald F. Dionne. Department of Materials Science and Engineering Massachusetts Institute of Technology

Magnetic Oxides. Gerald F. Dionne. Department of Materials Science and Engineering Massachusetts Institute of Technology Magnetic Oxides Gerald F. Dionne Department of Materials Science and Engineering Massachusetts Institute of Technology Spins in Solids Summer School University of Virginia Charlottesville, VA 21 June 2006

More information

Magnetic Circular Dichroism spectroscopy in epitaxial La 0.7 Sr 0.3 MnO 3 thin films

Magnetic Circular Dichroism spectroscopy in epitaxial La 0.7 Sr 0.3 MnO 3 thin films Magnetic Circular Dichroism spectroscopy in epitaxial La 0.7 Sr 0.3 MnO 3 thin films T. K. Nath 1 and J. R. Neal 2, G. A. Gehring 2 1 Dept. of Physics and Meteorology, Indian Institute Technology of Kharagpur,

More information

From Atoms to Materials: Predictive Theory and Simulations

From Atoms to Materials: Predictive Theory and Simulations From Atoms to Materials: Predictive Theory and Simulations Week 3 Lecture 4 Potentials for metals and semiconductors Ale Strachan strachan@purdue.edu School of Materials Engineering & Birck anotechnology

More information

Solid State Physics. The biggest part of physics in terms of the number of active researchers

Solid State Physics. The biggest part of physics in terms of the number of active researchers Solid State Physics The biggest part of physics in terms of the number of active researchers Fundamental science behind materials we use in technology A lot of cool effects that we understand: e.g. topological

More information

ELECTRONIC AND MAGNETIC PROPERTIES OF BERKELIUM MONONITRIDE BKN: A FIRST- PRINCIPLES STUDY

ELECTRONIC AND MAGNETIC PROPERTIES OF BERKELIUM MONONITRIDE BKN: A FIRST- PRINCIPLES STUDY ELECTRONIC AND MAGNETIC PROPERTIES OF BERKELIUM MONONITRIDE BKN: A FIRST- PRINCIPLES STUDY Gitanjali Pagare Department of Physics, Sarojini Naidu Govt. Girls P. G. Auto. College, Bhopal ( India) ABSTRACT

More information

Chapter 2 Experimental sources of intermolecular potentials

Chapter 2 Experimental sources of intermolecular potentials Chapter 2 Experimental sources of intermolecular potentials 2.1 Overview thermodynamical properties: heat of vaporization (Trouton s rule) crystal structures ionic crystals rare gas solids physico-chemical

More information

SYNTHESIS OF INORGANIC MATERIALS AND NANOMATERIALS. Pr. Charles Kappenstein LACCO, Laboratoire de Catalyse en Chimie Organique, Poitiers, France

SYNTHESIS OF INORGANIC MATERIALS AND NANOMATERIALS. Pr. Charles Kappenstein LACCO, Laboratoire de Catalyse en Chimie Organique, Poitiers, France SYNTHESIS OF INORGANIC MATERIALS AND NANOMATERIALS Pr. Charles Kappenstein LACCO, Laboratoire de Catalyse en Chimie Organique, Poitiers, France Outline IV - FORMATION OF SOLIDS FROM SOLUTIONS 1) Glass

More information

Structural and Optical Properties of ZnSe under Pressure

Structural and Optical Properties of ZnSe under Pressure www.stmjournals.com Structural and Optical Properties of ZnSe under Pressure A. Asad, A. Afaq* Center of Excellence in Solid State Physics, University of the Punjab Lahore-54590, Pakistan Abstract The

More information

per unit cell Motif: Re at (0, 0, 0); 3O at ( 1 / 2, 0), (0, 0, 1 / 2 ) Re: 6 (octahedral coordination) O: 2 (linear coordination) ReO 6

per unit cell Motif: Re at (0, 0, 0); 3O at ( 1 / 2, 0), (0, 0, 1 / 2 ) Re: 6 (octahedral coordination) O: 2 (linear coordination) ReO 6 Lattice: Primitive Cubic 1ReO 3 per unit cell Motif: Re at (0, 0, 0); 3O at ( 1 / 2, 0, 0), (0, 1 / 2, 0), (0, 0, 1 / 2 ) Re: 6 (octahedral coordination) O: 2 (linear coordination) ReO 6 octahedra share

More information

Size-dependent physical properties of nanostructures: Introduction

Size-dependent physical properties of nanostructures: Introduction Size-dependent physical properties of nanostructures: Introduction can protect you... Five times stronger than steel, this shiny beast is also twice as strong as any bullet stopping or bomb protection

More information

ISSN: ISO 9001:2008 Certified International Journal of Engineering and Innovative Technology (IJEIT) Volume 4, Issue 1, July 2014

ISSN: ISO 9001:2008 Certified International Journal of Engineering and Innovative Technology (IJEIT) Volume 4, Issue 1, July 2014 Structural and Electrical Properties of Sr - Substituted Perovskites Nano crystalline Lamno 3 G.N.Chaudhari, A.B.Bodade, D.K.Burghate Department of Chemistry, Shri Shivaji Science College, Amravati-444603

More information

Spreadsheet Applications for Materials Science

Spreadsheet Applications for Materials Science Spreadsheet Applications for Materials Science The Ionic Bond Introduction A good place to start the study of engineering materials is with the nature of the energies and forces involved in the bonding

More information

Condensed matter physics FKA091

Condensed matter physics FKA091 Condensed matter physics FKA091 Ermin Malic Department of Physics Chalmers University of Technology Henrik Johannesson Department of Physics University of Gothenburg Teaching assistants: Roland Jago &

More information

Anisotropic assessment of ultrasonic wave velocity and thermal conductivity in ErX (X:N, As)

Anisotropic assessment of ultrasonic wave velocity and thermal conductivity in ErX (X:N, As) Indian Journal of Pure & Applied Physics Vol. 54, January 216, pp. 4-45 Anisotropic assessment of ultrasonic wave velocity and thermal conductivity in ErX (X:N, As) Vyoma Bhalla 1, 2* & Devraj Singh 2

More information

Ultrafast X-ray Studies of Complex Materials: Science Challenges and Opportunities

Ultrafast X-ray Studies of Complex Materials: Science Challenges and Opportunities Ultrafast X-ray Studies of Complex Materials: Science Challenges and Opportunities Lawrence Berkeley National Laboratory Robert Schoenlein Materials Sciences Division - Chemical Sciences Division Ultrafast

More information

Kirori Mal College, University of Delhi

Kirori Mal College, University of Delhi Kirori Mal College, University of Delhi Title Dr. First Designation Address Phone No Office Residence ALOK ASSISTANT PROFESSOR Middle KUMAR SINGH Last E-175, DOUBLE STOREY,RAMESH NAGAR,NEW DELHI 011-25106889

More information

Academic profile: Positions Held:

Academic profile: Positions Held: Dr. S. S. UMARE Professor Department of Chemistry Visvesvaraya National Institute of Technology (Formerly VRCE), Nagpur 440 010 (M. S.) Phones : (O) 0712-2801316 Fax : 0712-2223230 E-mail: ssumare@chm.vnit.ac.in

More information

Cohesive energy of zinc blende (A III B V and A II B VI ) structured solids

Cohesive energy of zinc blende (A III B V and A II B VI ) structured solids Cohesive energy of zinc blende (A III B V and A II B VI ) structured solids A. S. Verma *,1, B. K. Sarkar 2 and V. K. Jindal 1 1 Department of Physics, Panjab University, Chandigarh, (India), 160014 2

More information

Roger Johnson Structure and Dynamics: Displacive phase transition Lecture 9

Roger Johnson Structure and Dynamics: Displacive phase transition Lecture 9 9.1. Summary In this Lecture we will consider structural phase transitions characterised by atomic displacements, which result in a low temperature structure that is distorted compared to a higher temperature,

More information