SlideShare a Scribd company logo
1 of 4
Download to read offline
Tanmoy Chakrabarty
Post-doctoral fellow
TIFR, Mumbai
400005 email: imtan90@gmail.com,
Academic Details
 Visiting post-doctorate fellow in TIFR, Mumbai
 M.Sc. Ph.D dual degree in Physics
Department of Physics, IIT Bombay, Powai, Mumbai, India (M.Sc.-2008, CPI- 7.21/10)
 B.Sc. in Physics (Hons) (2006, 56%)
R. K. Mission Vidyamandira, Belur Math, Howrah, WB, India
University: Calcutta University, Kolkata, India
 Higher Secondary (10+2) in Pure Science (2003, 84.2%)
Nabagram Vidyapith, Nabagram, Hooghly, west Bengal, India
Board: West Bengal Council of Higher Secondary Education, Kolkata
 Secondary Exam (2001, 90.13%)
Nabagram Vidyapith, Nabagram, Hooghly, west Bengal, India
Board: West Bengal Board of Secondary Education, Kolkata
Research Experience
 Research Scholar: Dept. of Physics, IIT Bombay, Mumbai, India (June 2008- Aug 2014) and
Teaching Assistant in the x-ray lab IIT Bombay
Supervisor: Prof. A.V. Mahajan, Dept. of Physics, IIT Bombay, Mumbai, India
 Post-doc fellow in TIFR: Department of Condensed matter Physics and material science, TIFR,
Mumbai, India (From May 2015 to present)
Host Professor: P L Paulose, Department of Condensed matter Physics and material science,
TIFR
Current Research Interest
Novel magnetic properties in low-dimensional geometrically frustrated S = 1/2 3d-based oxides: In
the last few decades special emphasis has been laid on low-dimensional spin systems such as chains, square
lattices, ladders, especially since they are intimately connected to the high-temperature cuprate
superconductors. In these low-dimensional systems quantum effects are more dominant for s=1/2 systems
because of their low value of spins. In the antiferromagnetic systems the scenario becomes even more
interesting since the non-fulfillment of simultaneous minimization of energy leads to many low lying
excited states. I have been working on new materials in these domains and studying their bulk and local
properties.
I prepare strongly correlated magnetic systems (mostly oxides) by standard solid state reaction method
using several furnaces and vacuum stations according to the requirements (especially for intermediate
valence state of oxide samples). Then I do the crystallographic studies of the prepared samples by the
PAnalytical X-ray Diffractometer which also has a provision to attach a low-temperature setup down to 4
K. Then I study the bulk properties of these systems using PPMS (Physical properties measurement
system-magnetization, heat capacity and resistivity) and SVSM (Squid-VSM). After that, the local
properties are studied by our solid state NMR setup consisting a 400MHz superconducting magnet
(VARIAN), a TECMAG/REDSTONE spectrometer and OXFORD cryostat with accessories. This was
installed in 2009. I was involved in the installation process and working with the system since then.
Here I give a brief description of the systems I worked. First, I mention the work I have done in my PhD.
I have worked in the 6,7
Li NMR measurements of La2Li0.5Cu0.5O4 which shows variation from Zhang-Rice
behavior with our Russian collaborators (A. A. Gippius et al.). This report is published in Phys. Rev. B 86,
241107 (2012) (Rapid Comm.)
On the quest of a novel low-dimensional magnetic system I worked on BaV3O8 where magnetic vanadium
ions (V4+
, S=1/2) are coupled with each other via the non-magnetic (V5+
, S=0) ones. From the bulk
measurements we find both short-range and long-range magnetic ordering in this system. Due to fast
relaxation we could not detect the magnetic vanadium but its presence was confirmed through the window
of the relaxation of the non-magnetic vanadium ions. The spin-spin relaxation confirms that there is a co-
existence of long-range ordered (LRO) and non-LRO regions below the long-range ordering temperature.
This work has been published in Phys Rev. B 88, 014433 (2013)
Another vanadium-based system we studied is Li2ZnV3O8, which is a Zn-doped LiV2O4 system with all the
vanadium ions are in S=1/2 magnetic state. The bulk measurements show no magnetic LRO but a spin-
glass like transition is observed (ZFC-FC split). We confirmed from our NMR measurements that unlike
other doped LiV2O4 systems, lithium is weakly couples with vanadium ions although there is a presence of
glassy anomaly like pristine LiV2O4 and other doped LiV2O4 systems. This work has been published in J.
Phys: Cond. Mat. 26, 265601 (2014)
Third vanadium-based compound which I have done in my PhD is Zn3V3O8, which shows cluster spin-
glass behavior and we have studied its spin-glass characteristics and to explore more we carried out further
experiments and observed magnetic relaxation, memory and aging phenomena which are thought to be
typical characteristics of spin glass dynamics. This work is published in J. Phys: Cond. Mat. 26, 405601
(2014)
From 2015 onwards, I have joined in TIFR Mumbai as a post-doctoral visiting fellow and was involved in
successfully building a solid-state NMR setup with my host Prof. P L Paulose. After that, we have carried
out a comparative bulk and NMR study of two ruthanate compounds, Ca3LiRuO6 and Ca3NaRuO6, with
similar A3ATO6-type (A = Ca, Sr; A′ = Li, Na, TM; T = TM) of structure, with the NMR probe we built.
Out of these two compounds, Ca3LiRuO6 is a weak ferromagnet with a magnetic ordering temperature of
115 K. The 7
Li NMR linewidth of Ca3LiRuO6 displays a broad shoulder above the magnetic ordering
temperature. Anomalous shoulder of this type is observed in the magnetic susceptibility data also. The
origin of these phenomena is not clear but could possibly be attributed to low dimensional magnetism. A
contrasting magnetic behavior is seen in Ca3NaRuO6, an antiferromagnet with a transition temperature at
87 K. The heat capacity of both compounds show a λ-type anomaly at respective magnetic transition
temperatures. However, in both the systems the entropy change (ΔS) is much less than that of an ordered S
= 3/2 system. The NMR study shows that the Knight shift is proportional to the magnetic susceptibility.
Also, in Ca3NaRuO6, the Knight shift and the linewidth of the spectra change differently compared to
Ca3LiRuO6.
This work is very recently accepted in Journal of physics: Condensed matter
We have also carried out bulk and NMR studies on three more strongly correlated low-dimensional spin
systems here in TIFR, the manuscript of these are under preparation now.
Publications
Accepted/published/under review in journals
1. Magnetic Studies on a New S  =  1/2 Vanadium Based (V4+
) Geometrically Frustrated System
(BaV3O8): Tanmoy Chakrabarty and A.V. Mahajan, AIP Conf. Proc. 1349, 1199 (2011)
2. Direct evidence of non-Zhang-Rice Cu3+
centers in La2Li0.5Cu0.5O4: A. S. Moskvin, A. A. Gippius,
A. V. Tkachev, A.V. Mahajan, T. Chakrabarty, I. A. Presniakov, A. V. Sobolev and G.
Demazeau, Phys. Rev. B 86, 241107 (2012) (Rapid Comm.)
3. BaV3O8: A possible Majumdar-Ghosh system with S=1/2 , T. Chakarabarty: A.V. Mahajan, A.
Gippius, A. V. Tkachev, N.Buettgen, W. Kraetschmer, Phys. Rev. B 88, 014433 (2013)
4. Li2ZnV3O8: a vanadium-based geometrically frustrated spinel system, T Chakrabarty, A V
Mahajan and B Koteswararao, J. Phys.: Condens. Matter 26, 265601(2014)
5. Cluster spin glass behavior in geometrically frustrated Zn3V3O8: T. Chakrabarty, A. V. Mahajan
and S. Kundu, J. Phys.: Condens. Matter 26, 405601(2014)
6. Comparative NMR studies on Ca3LiRuO6 and Ca3NaRuO6, T Chakrabarty and P L Paulose
(Accepted in J. Phys.: Condens. Matter, 2016)
Presentations
Conference, School Workshop and Academic visits
1. Attended Indian Condensed Matter Workshop held in Mahabaleshwar during Dec 9-22, 2008
2. Presented poster at the Indo-US Workshop on Advanced Magnetic Materials and their application,
1-4th
March 2009 held at Mumbai, India.
3. Attended Workshop on Cryogenics and Physics at Low Temperature, on 9th
July 2009, held at
TIFR, Mumbai, India.
4. Presented poster at the International Conference on Magnetism, Superconductivity and Phase
Transition in Novel and Complex Materials (MSM-2009), 11-14th
November, 2009, held at
Kolkata, India.
5. Contributed talk on ‘Study of a low-dimensional geometrically frustrated magnetic systems’ at
SYMPHY 2013, IIT Bombay (4th
April 2013)
6. Attended and presented poster in the Lowtherm final workshop ("quantum magnets 2013"
Advances in quantum magnets – dynamics), Kolymbari, Crete, Greece
7. Attended and given an oral presentation in JCNS (Jülich Centre for Neutron Science) workshop
focusing on Trends and Perspectives in Neutron Scattering: Magnetism and Correlated Electron
Systems from 7-10th
October, 2013 at Tutzing, Germany
8. 32nd
Young Physicists Colloquium, 21-22 August, 2014, Kolkata, West Bengal, India
9. Presented Poster in the Workshop on current trends in frustrated magnetism 9-13 February,
2015 organized by International Centre for Theoretical Physics (ICTP) in JNU, New Delhi
10. Visited Max Planck -Institute for Chemical Physics of Solids in Dresden, Germany for 2 weeks in
2015 and given an oral presentation
11. Visited University of Pavia, Italy in 2015 and given an oral presentation
12. Visited ETH Zurich, Switzerland in 2015 and given an oral presentation
Teaching Experience
 Guided four M.Sc. (Mr. Kousik Sen, Mr. Tathamay Basu, Mr. Debashish and Mr. Rajesh) students
of Dept. of Physics, IIT Bombay for their respective Master’s thesis project.
 Teaching Assistant in General Physics Laboratory for 1st
year B.Tech. students at Dept. of
Physics, IIT Bombay.
 Teaching Assistant in General Physics Laboratory for 1st
year M.Sc. students at Dept. of Physics,
IIT Bombay.
 Teaching Assistant in Solid State Physics laboratory for 3rd
year B.Tech. students and 2nd
year
M.Sc. students at Dept. of Physics, IIT Bombay.
Demonstration in scientific exhibitions
Demonstrated “superconductivity and magnetic levitation” in ‘IIT Bombay Techfest” ( 2011-2013)
Techfest Homepage: http://www.techfest.org/
Awards and Achievements
 Secured 78th
all India rank in JAM-2006 (conducted by all IITs) among more than 4000 students.
 Secured 2183th
rank among more than 100,000 students appeared in WBJEE-2002 conducted by
WBUT, Kolkata, India.
 Stood 44th
in 10th
level board exam.
 Recipient of National Scholarship based on performance in 10th
and 10+2 level board exam.
Research Skills:
 Theoretical and operational knowledge and more than five years of experience in solid state NMR
techniques since 2010.
 Regular user of PPMS (Physical properties measurement system-magnetization, heat capacity and
resistivity), SVSM (Squid-VSM) from 2008
 Operator PAnalytical X-ray Diffractometer from 2009-2011
 Operational knowledge in vacuum techniques ( Turbo pump, Diffusion pump, rotary pump)
 Prepared around 15 compounds to study their physical properties in standard solid state reaction
method and expertise in preparing vanadium-based systems.
References
Prof. A. V. Mahajan (PhD guide)
Professor,
Department of Physics, Ph No: +91-22-25767573
Indian Institute of Technology Bombay, Fax: +91-22-25723480
Powai, Mumbai - 400076, India email: mahajan@phy.iitb.ac.in
Homepage: http://www.phy.iitb.ac.in/doku/doku.php/faculty/mahajan/home
Prof. A. A. Gippius (Collaborator)
Professor
Faculty of Physics,
Lomonosov Moscow State University,
Moscow 119991, Russia email: gippius@mail.ru
Prof. K. G. Suresh (PhD research progress committee member)
Professor,
Department of Physics, Ph No: +91-22-25767559
Indian Institute of Technology Bombay, Fax: +91-22-25723480
Powai, Mumbai - 400076, India email: suresh@phy.iitb.ac.in
Homepage: http://www.phy.iitb.ac.in/doku/doku.php/faculty/suresh/home
Prof. P.L. Paulose (Host Professor in TIFR)
Professor,
Condensed Matter Physics and Materials Science
Office : A-171
Office Phone : 22782412
Lab : CG-28
Lab Phone : 22782434
Email : paulose@tifr.res.in

More Related Content

What's hot

Bridging length and time scales in biomolecular systems
Bridging length and time scales in biomolecular systemsBridging length and time scales in biomolecular systems
Bridging length and time scales in biomolecular systemsuvacolloquium
 
35 Charged particle detection at GRAAL - Radiation Effects & Defects in Solid...
35 Charged particle detection at GRAAL - Radiation Effects & Defects in Solid...35 Charged particle detection at GRAAL - Radiation Effects & Defects in Solid...
35 Charged particle detection at GRAAL - Radiation Effects & Defects in Solid...Cristian Randieri PhD
 
Radio chemical method of analysis
Radio chemical method of analysis Radio chemical method of analysis
Radio chemical method of analysis MedhaThakur2
 
Rapid analysis of polymers and petroleum by Ion-mobility mass spectrometry
Rapid analysis of polymers and petroleum by Ion-mobility mass spectrometryRapid analysis of polymers and petroleum by Ion-mobility mass spectrometry
Rapid analysis of polymers and petroleum by Ion-mobility mass spectrometryWaters Corporation - Chemical Materials
 
Maldi tof spectrometry
Maldi tof spectrometryMaldi tof spectrometry
Maldi tof spectrometryzohairkhan22
 
IJERD (www.ijerd.com) International Journal of Engineering Research and Devel...
IJERD (www.ijerd.com) International Journal of Engineering Research and Devel...IJERD (www.ijerd.com) International Journal of Engineering Research and Devel...
IJERD (www.ijerd.com) International Journal of Engineering Research and Devel...IJERD Editor
 
(Preprint No. 4) (There's A light Beam Velocity = 1.16 mkm per second)
(Preprint No. 4) (There's A light Beam Velocity = 1.16 mkm per second)(Preprint No. 4) (There's A light Beam Velocity = 1.16 mkm per second)
(Preprint No. 4) (There's A light Beam Velocity = 1.16 mkm per second)Gerges francis
 
2003 self-organization processes in impurity subsystem of solid solutions
2003 self-organization processes in impurity subsystem of solid solutions2003 self-organization processes in impurity subsystem of solid solutions
2003 self-organization processes in impurity subsystem of solid solutionsДарья Орлова
 
Planet Orbital Distance Equation
Planet Orbital Distance Equation Planet Orbital Distance Equation
Planet Orbital Distance Equation Gerges francis
 
Protons Relaxation and Temperature Dependence Due To Tunneling Methyl Group
Protons Relaxation and Temperature Dependence Due To Tunneling Methyl GroupProtons Relaxation and Temperature Dependence Due To Tunneling Methyl Group
Protons Relaxation and Temperature Dependence Due To Tunneling Methyl GroupIJERA Editor
 
On the-mechanism-of-proton-conductivity-in-h-sub3sub o-sbteo-sub6sub_2012_jou...
On the-mechanism-of-proton-conductivity-in-h-sub3sub o-sbteo-sub6sub_2012_jou...On the-mechanism-of-proton-conductivity-in-h-sub3sub o-sbteo-sub6sub_2012_jou...
On the-mechanism-of-proton-conductivity-in-h-sub3sub o-sbteo-sub6sub_2012_jou...Javier Lemus Godoy
 
Principles of Multiscale Modelling of Materials
Principles of Multiscale Modelling of Materials  Principles of Multiscale Modelling of Materials
Principles of Multiscale Modelling of Materials Altair
 
Large hadron collider
Large hadron colliderLarge hadron collider
Large hadron collideranoop kp
 
Cold atoms trapped by nanostructures
Cold atoms trapped by nanostructuresCold atoms trapped by nanostructures
Cold atoms trapped by nanostructuresGabriel O'Brien
 
Mass spectrometry
Mass spectrometryMass spectrometry
Mass spectrometryRAVI RANJAN
 
PH600 Project report
PH600 Project reportPH600 Project report
PH600 Project reportLuke Moore
 

What's hot (20)

Bridging length and time scales in biomolecular systems
Bridging length and time scales in biomolecular systemsBridging length and time scales in biomolecular systems
Bridging length and time scales in biomolecular systems
 
35 Charged particle detection at GRAAL - Radiation Effects & Defects in Solid...
35 Charged particle detection at GRAAL - Radiation Effects & Defects in Solid...35 Charged particle detection at GRAAL - Radiation Effects & Defects in Solid...
35 Charged particle detection at GRAAL - Radiation Effects & Defects in Solid...
 
MALDI
MALDIMALDI
MALDI
 
Radio chemical method of analysis
Radio chemical method of analysis Radio chemical method of analysis
Radio chemical method of analysis
 
Rapid analysis of polymers and petroleum by Ion-mobility mass spectrometry
Rapid analysis of polymers and petroleum by Ion-mobility mass spectrometryRapid analysis of polymers and petroleum by Ion-mobility mass spectrometry
Rapid analysis of polymers and petroleum by Ion-mobility mass spectrometry
 
Maldi tof spectrometry
Maldi tof spectrometryMaldi tof spectrometry
Maldi tof spectrometry
 
XRD Proposal
XRD ProposalXRD Proposal
XRD Proposal
 
Some aspects of Fractons
Some aspects of FractonsSome aspects of Fractons
Some aspects of Fractons
 
Ms basics
Ms basicsMs basics
Ms basics
 
IJERD (www.ijerd.com) International Journal of Engineering Research and Devel...
IJERD (www.ijerd.com) International Journal of Engineering Research and Devel...IJERD (www.ijerd.com) International Journal of Engineering Research and Devel...
IJERD (www.ijerd.com) International Journal of Engineering Research and Devel...
 
(Preprint No. 4) (There's A light Beam Velocity = 1.16 mkm per second)
(Preprint No. 4) (There's A light Beam Velocity = 1.16 mkm per second)(Preprint No. 4) (There's A light Beam Velocity = 1.16 mkm per second)
(Preprint No. 4) (There's A light Beam Velocity = 1.16 mkm per second)
 
2003 self-organization processes in impurity subsystem of solid solutions
2003 self-organization processes in impurity subsystem of solid solutions2003 self-organization processes in impurity subsystem of solid solutions
2003 self-organization processes in impurity subsystem of solid solutions
 
Planet Orbital Distance Equation
Planet Orbital Distance Equation Planet Orbital Distance Equation
Planet Orbital Distance Equation
 
Protons Relaxation and Temperature Dependence Due To Tunneling Methyl Group
Protons Relaxation and Temperature Dependence Due To Tunneling Methyl GroupProtons Relaxation and Temperature Dependence Due To Tunneling Methyl Group
Protons Relaxation and Temperature Dependence Due To Tunneling Methyl Group
 
On the-mechanism-of-proton-conductivity-in-h-sub3sub o-sbteo-sub6sub_2012_jou...
On the-mechanism-of-proton-conductivity-in-h-sub3sub o-sbteo-sub6sub_2012_jou...On the-mechanism-of-proton-conductivity-in-h-sub3sub o-sbteo-sub6sub_2012_jou...
On the-mechanism-of-proton-conductivity-in-h-sub3sub o-sbteo-sub6sub_2012_jou...
 
Principles of Multiscale Modelling of Materials
Principles of Multiscale Modelling of Materials  Principles of Multiscale Modelling of Materials
Principles of Multiscale Modelling of Materials
 
Large hadron collider
Large hadron colliderLarge hadron collider
Large hadron collider
 
Cold atoms trapped by nanostructures
Cold atoms trapped by nanostructuresCold atoms trapped by nanostructures
Cold atoms trapped by nanostructures
 
Mass spectrometry
Mass spectrometryMass spectrometry
Mass spectrometry
 
PH600 Project report
PH600 Project reportPH600 Project report
PH600 Project report
 

Viewers also liked

Viewers also liked (8)

Quantum formula sheet
Quantum formula sheetQuantum formula sheet
Quantum formula sheet
 
tifr report
tifr reporttifr report
tifr report
 
2016.06.21 gmm csic NanoFrontMag
2016.06.21 gmm csic NanoFrontMag2016.06.21 gmm csic NanoFrontMag
2016.06.21 gmm csic NanoFrontMag
 
TIFR_Report
TIFR_ReportTIFR_Report
TIFR_Report
 
Czeroc ppt slideshow
Czeroc ppt slideshowCzeroc ppt slideshow
Czeroc ppt slideshow
 
ASBTE_poster_march20-final (1)
ASBTE_poster_march20-final (1)ASBTE_poster_march20-final (1)
ASBTE_poster_march20-final (1)
 
nano wire
nano wirenano wire
nano wire
 
Ferrites
Ferrites Ferrites
Ferrites
 

Similar to Post-doc Tanmoy's CV

Magnon crystallization in kagomé antiferromagnets
Magnon crystallization in kagomé antiferromagnetsMagnon crystallization in kagomé antiferromagnets
Magnon crystallization in kagomé antiferromagnetsRyutaro Okuma
 
Laboratory Raman spectroscopy ISP NASU
Laboratory Raman spectroscopy ISP NASULaboratory Raman spectroscopy ISP NASU
Laboratory Raman spectroscopy ISP NASUЮлия Деева
 
Probing Molecular Electronic Structure Using High Harmonic Generation Tomography
Probing Molecular Electronic Structure Using High Harmonic Generation TomographyProbing Molecular Electronic Structure Using High Harmonic Generation Tomography
Probing Molecular Electronic Structure Using High Harmonic Generation TomographyChelsey Crosse
 
Ion-acoustic rogue waves in multi-ion plasmas
Ion-acoustic rogue waves in multi-ion plasmasIon-acoustic rogue waves in multi-ion plasmas
Ion-acoustic rogue waves in multi-ion plasmasMehedi Hassan
 
Opportunities for students
Opportunities for students Opportunities for students
Opportunities for students Rene Kotze
 
Kinetic growth of binary compounds by reactive sputtering magnetron
Kinetic growth of binary compounds by reactive sputtering magnetronKinetic growth of binary compounds by reactive sputtering magnetron
Kinetic growth of binary compounds by reactive sputtering magnetronJavier García Molleja
 
Like-CV-2016
Like-CV-2016Like-CV-2016
Like-CV-2016Ke Li
 
Aip pg book of abstracts
Aip pg book of abstractsAip pg book of abstracts
Aip pg book of abstractsSiddartha Verma
 
Advantages And Disadvantages Of Nuclear Magnetic Resonance Spectroscopy As A ...
Advantages And Disadvantages Of Nuclear Magnetic Resonance Spectroscopy As A ...Advantages And Disadvantages Of Nuclear Magnetic Resonance Spectroscopy As A ...
Advantages And Disadvantages Of Nuclear Magnetic Resonance Spectroscopy As A ...Daniel Wachtel
 
BT631-11-x-ray_crystallography_introduction
BT631-11-x-ray_crystallography_introductionBT631-11-x-ray_crystallography_introduction
BT631-11-x-ray_crystallography_introductionRajesh G
 
Quantum-systems investigations vs optical-systems ones
Quantum-systems investigations vs optical-systems onesQuantum-systems investigations vs optical-systems ones
Quantum-systems investigations vs optical-systems onesOrchidea Maria Lecian
 
Introduction to nanoscience and nanotechnology
Introduction to nanoscience and nanotechnologyIntroduction to nanoscience and nanotechnology
Introduction to nanoscience and nanotechnologyaimanmukhtar1
 
Mass spectrometry
Mass spectrometryMass spectrometry
Mass spectrometrySadiq Rahim
 

Similar to Post-doc Tanmoy's CV (20)

Bput
BputBput
Bput
 
Bput
BputBput
Bput
 
Mybput
MybputMybput
Mybput
 
Aa16869 11
Aa16869 11Aa16869 11
Aa16869 11
 
Magnon crystallization in kagomé antiferromagnets
Magnon crystallization in kagomé antiferromagnetsMagnon crystallization in kagomé antiferromagnets
Magnon crystallization in kagomé antiferromagnets
 
Laboratory Raman spectroscopy ISP NASU
Laboratory Raman spectroscopy ISP NASULaboratory Raman spectroscopy ISP NASU
Laboratory Raman spectroscopy ISP NASU
 
Espectrometría de Masas Atómica
Espectrometría de Masas AtómicaEspectrometría de Masas Atómica
Espectrometría de Masas Atómica
 
BSc Thesis
BSc ThesisBSc Thesis
BSc Thesis
 
Probing Molecular Electronic Structure Using High Harmonic Generation Tomography
Probing Molecular Electronic Structure Using High Harmonic Generation TomographyProbing Molecular Electronic Structure Using High Harmonic Generation Tomography
Probing Molecular Electronic Structure Using High Harmonic Generation Tomography
 
Ion-acoustic rogue waves in multi-ion plasmas
Ion-acoustic rogue waves in multi-ion plasmasIon-acoustic rogue waves in multi-ion plasmas
Ion-acoustic rogue waves in multi-ion plasmas
 
Opportunities for students
Opportunities for students Opportunities for students
Opportunities for students
 
Kinetic growth of binary compounds by reactive sputtering magnetron
Kinetic growth of binary compounds by reactive sputtering magnetronKinetic growth of binary compounds by reactive sputtering magnetron
Kinetic growth of binary compounds by reactive sputtering magnetron
 
Like-CV-2016
Like-CV-2016Like-CV-2016
Like-CV-2016
 
Nature12917
Nature12917Nature12917
Nature12917
 
Aip pg book of abstracts
Aip pg book of abstractsAip pg book of abstracts
Aip pg book of abstracts
 
Advantages And Disadvantages Of Nuclear Magnetic Resonance Spectroscopy As A ...
Advantages And Disadvantages Of Nuclear Magnetic Resonance Spectroscopy As A ...Advantages And Disadvantages Of Nuclear Magnetic Resonance Spectroscopy As A ...
Advantages And Disadvantages Of Nuclear Magnetic Resonance Spectroscopy As A ...
 
BT631-11-x-ray_crystallography_introduction
BT631-11-x-ray_crystallography_introductionBT631-11-x-ray_crystallography_introduction
BT631-11-x-ray_crystallography_introduction
 
Quantum-systems investigations vs optical-systems ones
Quantum-systems investigations vs optical-systems onesQuantum-systems investigations vs optical-systems ones
Quantum-systems investigations vs optical-systems ones
 
Introduction to nanoscience and nanotechnology
Introduction to nanoscience and nanotechnologyIntroduction to nanoscience and nanotechnology
Introduction to nanoscience and nanotechnology
 
Mass spectrometry
Mass spectrometryMass spectrometry
Mass spectrometry
 

Post-doc Tanmoy's CV

  • 1. Tanmoy Chakrabarty Post-doctoral fellow TIFR, Mumbai 400005 email: imtan90@gmail.com, Academic Details  Visiting post-doctorate fellow in TIFR, Mumbai  M.Sc. Ph.D dual degree in Physics Department of Physics, IIT Bombay, Powai, Mumbai, India (M.Sc.-2008, CPI- 7.21/10)  B.Sc. in Physics (Hons) (2006, 56%) R. K. Mission Vidyamandira, Belur Math, Howrah, WB, India University: Calcutta University, Kolkata, India  Higher Secondary (10+2) in Pure Science (2003, 84.2%) Nabagram Vidyapith, Nabagram, Hooghly, west Bengal, India Board: West Bengal Council of Higher Secondary Education, Kolkata  Secondary Exam (2001, 90.13%) Nabagram Vidyapith, Nabagram, Hooghly, west Bengal, India Board: West Bengal Board of Secondary Education, Kolkata Research Experience  Research Scholar: Dept. of Physics, IIT Bombay, Mumbai, India (June 2008- Aug 2014) and Teaching Assistant in the x-ray lab IIT Bombay Supervisor: Prof. A.V. Mahajan, Dept. of Physics, IIT Bombay, Mumbai, India  Post-doc fellow in TIFR: Department of Condensed matter Physics and material science, TIFR, Mumbai, India (From May 2015 to present) Host Professor: P L Paulose, Department of Condensed matter Physics and material science, TIFR Current Research Interest Novel magnetic properties in low-dimensional geometrically frustrated S = 1/2 3d-based oxides: In the last few decades special emphasis has been laid on low-dimensional spin systems such as chains, square lattices, ladders, especially since they are intimately connected to the high-temperature cuprate superconductors. In these low-dimensional systems quantum effects are more dominant for s=1/2 systems because of their low value of spins. In the antiferromagnetic systems the scenario becomes even more interesting since the non-fulfillment of simultaneous minimization of energy leads to many low lying excited states. I have been working on new materials in these domains and studying their bulk and local properties. I prepare strongly correlated magnetic systems (mostly oxides) by standard solid state reaction method using several furnaces and vacuum stations according to the requirements (especially for intermediate valence state of oxide samples). Then I do the crystallographic studies of the prepared samples by the PAnalytical X-ray Diffractometer which also has a provision to attach a low-temperature setup down to 4 K. Then I study the bulk properties of these systems using PPMS (Physical properties measurement system-magnetization, heat capacity and resistivity) and SVSM (Squid-VSM). After that, the local properties are studied by our solid state NMR setup consisting a 400MHz superconducting magnet
  • 2. (VARIAN), a TECMAG/REDSTONE spectrometer and OXFORD cryostat with accessories. This was installed in 2009. I was involved in the installation process and working with the system since then. Here I give a brief description of the systems I worked. First, I mention the work I have done in my PhD. I have worked in the 6,7 Li NMR measurements of La2Li0.5Cu0.5O4 which shows variation from Zhang-Rice behavior with our Russian collaborators (A. A. Gippius et al.). This report is published in Phys. Rev. B 86, 241107 (2012) (Rapid Comm.) On the quest of a novel low-dimensional magnetic system I worked on BaV3O8 where magnetic vanadium ions (V4+ , S=1/2) are coupled with each other via the non-magnetic (V5+ , S=0) ones. From the bulk measurements we find both short-range and long-range magnetic ordering in this system. Due to fast relaxation we could not detect the magnetic vanadium but its presence was confirmed through the window of the relaxation of the non-magnetic vanadium ions. The spin-spin relaxation confirms that there is a co- existence of long-range ordered (LRO) and non-LRO regions below the long-range ordering temperature. This work has been published in Phys Rev. B 88, 014433 (2013) Another vanadium-based system we studied is Li2ZnV3O8, which is a Zn-doped LiV2O4 system with all the vanadium ions are in S=1/2 magnetic state. The bulk measurements show no magnetic LRO but a spin- glass like transition is observed (ZFC-FC split). We confirmed from our NMR measurements that unlike other doped LiV2O4 systems, lithium is weakly couples with vanadium ions although there is a presence of glassy anomaly like pristine LiV2O4 and other doped LiV2O4 systems. This work has been published in J. Phys: Cond. Mat. 26, 265601 (2014) Third vanadium-based compound which I have done in my PhD is Zn3V3O8, which shows cluster spin- glass behavior and we have studied its spin-glass characteristics and to explore more we carried out further experiments and observed magnetic relaxation, memory and aging phenomena which are thought to be typical characteristics of spin glass dynamics. This work is published in J. Phys: Cond. Mat. 26, 405601 (2014) From 2015 onwards, I have joined in TIFR Mumbai as a post-doctoral visiting fellow and was involved in successfully building a solid-state NMR setup with my host Prof. P L Paulose. After that, we have carried out a comparative bulk and NMR study of two ruthanate compounds, Ca3LiRuO6 and Ca3NaRuO6, with similar A3ATO6-type (A = Ca, Sr; A′ = Li, Na, TM; T = TM) of structure, with the NMR probe we built. Out of these two compounds, Ca3LiRuO6 is a weak ferromagnet with a magnetic ordering temperature of 115 K. The 7 Li NMR linewidth of Ca3LiRuO6 displays a broad shoulder above the magnetic ordering temperature. Anomalous shoulder of this type is observed in the magnetic susceptibility data also. The origin of these phenomena is not clear but could possibly be attributed to low dimensional magnetism. A contrasting magnetic behavior is seen in Ca3NaRuO6, an antiferromagnet with a transition temperature at 87 K. The heat capacity of both compounds show a λ-type anomaly at respective magnetic transition temperatures. However, in both the systems the entropy change (ΔS) is much less than that of an ordered S = 3/2 system. The NMR study shows that the Knight shift is proportional to the magnetic susceptibility. Also, in Ca3NaRuO6, the Knight shift and the linewidth of the spectra change differently compared to Ca3LiRuO6. This work is very recently accepted in Journal of physics: Condensed matter We have also carried out bulk and NMR studies on three more strongly correlated low-dimensional spin systems here in TIFR, the manuscript of these are under preparation now. Publications Accepted/published/under review in journals 1. Magnetic Studies on a New S  =  1/2 Vanadium Based (V4+ ) Geometrically Frustrated System (BaV3O8): Tanmoy Chakrabarty and A.V. Mahajan, AIP Conf. Proc. 1349, 1199 (2011)
  • 3. 2. Direct evidence of non-Zhang-Rice Cu3+ centers in La2Li0.5Cu0.5O4: A. S. Moskvin, A. A. Gippius, A. V. Tkachev, A.V. Mahajan, T. Chakrabarty, I. A. Presniakov, A. V. Sobolev and G. Demazeau, Phys. Rev. B 86, 241107 (2012) (Rapid Comm.) 3. BaV3O8: A possible Majumdar-Ghosh system with S=1/2 , T. Chakarabarty: A.V. Mahajan, A. Gippius, A. V. Tkachev, N.Buettgen, W. Kraetschmer, Phys. Rev. B 88, 014433 (2013) 4. Li2ZnV3O8: a vanadium-based geometrically frustrated spinel system, T Chakrabarty, A V Mahajan and B Koteswararao, J. Phys.: Condens. Matter 26, 265601(2014) 5. Cluster spin glass behavior in geometrically frustrated Zn3V3O8: T. Chakrabarty, A. V. Mahajan and S. Kundu, J. Phys.: Condens. Matter 26, 405601(2014) 6. Comparative NMR studies on Ca3LiRuO6 and Ca3NaRuO6, T Chakrabarty and P L Paulose (Accepted in J. Phys.: Condens. Matter, 2016) Presentations Conference, School Workshop and Academic visits 1. Attended Indian Condensed Matter Workshop held in Mahabaleshwar during Dec 9-22, 2008 2. Presented poster at the Indo-US Workshop on Advanced Magnetic Materials and their application, 1-4th March 2009 held at Mumbai, India. 3. Attended Workshop on Cryogenics and Physics at Low Temperature, on 9th July 2009, held at TIFR, Mumbai, India. 4. Presented poster at the International Conference on Magnetism, Superconductivity and Phase Transition in Novel and Complex Materials (MSM-2009), 11-14th November, 2009, held at Kolkata, India. 5. Contributed talk on ‘Study of a low-dimensional geometrically frustrated magnetic systems’ at SYMPHY 2013, IIT Bombay (4th April 2013) 6. Attended and presented poster in the Lowtherm final workshop ("quantum magnets 2013" Advances in quantum magnets – dynamics), Kolymbari, Crete, Greece 7. Attended and given an oral presentation in JCNS (Jülich Centre for Neutron Science) workshop focusing on Trends and Perspectives in Neutron Scattering: Magnetism and Correlated Electron Systems from 7-10th October, 2013 at Tutzing, Germany 8. 32nd Young Physicists Colloquium, 21-22 August, 2014, Kolkata, West Bengal, India 9. Presented Poster in the Workshop on current trends in frustrated magnetism 9-13 February, 2015 organized by International Centre for Theoretical Physics (ICTP) in JNU, New Delhi 10. Visited Max Planck -Institute for Chemical Physics of Solids in Dresden, Germany for 2 weeks in 2015 and given an oral presentation 11. Visited University of Pavia, Italy in 2015 and given an oral presentation 12. Visited ETH Zurich, Switzerland in 2015 and given an oral presentation Teaching Experience  Guided four M.Sc. (Mr. Kousik Sen, Mr. Tathamay Basu, Mr. Debashish and Mr. Rajesh) students of Dept. of Physics, IIT Bombay for their respective Master’s thesis project.  Teaching Assistant in General Physics Laboratory for 1st year B.Tech. students at Dept. of Physics, IIT Bombay.  Teaching Assistant in General Physics Laboratory for 1st year M.Sc. students at Dept. of Physics, IIT Bombay.  Teaching Assistant in Solid State Physics laboratory for 3rd year B.Tech. students and 2nd year M.Sc. students at Dept. of Physics, IIT Bombay. Demonstration in scientific exhibitions Demonstrated “superconductivity and magnetic levitation” in ‘IIT Bombay Techfest” ( 2011-2013) Techfest Homepage: http://www.techfest.org/
  • 4. Awards and Achievements  Secured 78th all India rank in JAM-2006 (conducted by all IITs) among more than 4000 students.  Secured 2183th rank among more than 100,000 students appeared in WBJEE-2002 conducted by WBUT, Kolkata, India.  Stood 44th in 10th level board exam.  Recipient of National Scholarship based on performance in 10th and 10+2 level board exam. Research Skills:  Theoretical and operational knowledge and more than five years of experience in solid state NMR techniques since 2010.  Regular user of PPMS (Physical properties measurement system-magnetization, heat capacity and resistivity), SVSM (Squid-VSM) from 2008  Operator PAnalytical X-ray Diffractometer from 2009-2011  Operational knowledge in vacuum techniques ( Turbo pump, Diffusion pump, rotary pump)  Prepared around 15 compounds to study their physical properties in standard solid state reaction method and expertise in preparing vanadium-based systems. References Prof. A. V. Mahajan (PhD guide) Professor, Department of Physics, Ph No: +91-22-25767573 Indian Institute of Technology Bombay, Fax: +91-22-25723480 Powai, Mumbai - 400076, India email: mahajan@phy.iitb.ac.in Homepage: http://www.phy.iitb.ac.in/doku/doku.php/faculty/mahajan/home Prof. A. A. Gippius (Collaborator) Professor Faculty of Physics, Lomonosov Moscow State University, Moscow 119991, Russia email: gippius@mail.ru Prof. K. G. Suresh (PhD research progress committee member) Professor, Department of Physics, Ph No: +91-22-25767559 Indian Institute of Technology Bombay, Fax: +91-22-25723480 Powai, Mumbai - 400076, India email: suresh@phy.iitb.ac.in Homepage: http://www.phy.iitb.ac.in/doku/doku.php/faculty/suresh/home Prof. P.L. Paulose (Host Professor in TIFR) Professor, Condensed Matter Physics and Materials Science Office : A-171 Office Phone : 22782412 Lab : CG-28 Lab Phone : 22782434 Email : paulose@tifr.res.in