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Remarkable 3D MAX Phases &
2D Wonder Materials MXenes
A.K.M. A. Islam
Professor of Physics (Retd.), Rajshahi University
8-10 March 2018 BPS Conference-2018 1
Outline
 3D MAX Phase Materials (Nanolaminate):
- Exciting new class of materials – Why ?
- MAX phases: Bridging the gap between
metals & ceramics
- Applications
 Our Research on MAX Phases 
- Prediction of yet unobserved phases
- Substitution – strengthening study:
(Ti, V)2AlC2 etc.
- Superconducting MAX phases
 2D MXenes derived from 3D MAX
Phases
- Stories of new wonder materials
8-10 March 2018 BPS Conference-2018 2
Any shape that only has a surface area is a 2-D
shape while shapes with volume are 3-D shapes.
Lab: A K M A Islam
Out of 91
3D MAX Phase
Formula: Mn+1AXn
– M is an early transition metal
– A is an A-group element
– X is either C or N
8-10 March 2018 BPS Conference-2018 3
Now > 70 phases-- most discovered &
produced in powder form in the 60’s by
H. Nowotny & coworkers.
First fabricated in bulk
& characterized
(Dr. Barsoum Group at Drexel University, USA)
MAX Materials
Ti2InN
Reactive hot-pressing of a ZrH2, Al
& C powder mixture MAX Zr2AlC
Exciting MAX Phases
8-10 March 2018 BPS Conference-2018 4
The term “MAX phases” was coined in the late 1990s.
Renewed interest in MAX Phases after Barsoum & El-Raghy’s
report in 1996 on the synthesis of phase-pure bulk T3SiC2
samples & their unusual combination of properties.
Since then, Research on the MAX phases has exploded.
According to ISI, to date > 1,200 papers have been published on
one MAX phase alone, T3SiC2, with roughly half of those
published in the past 6 years.
Exciting MAX: Bridging the Gap between
Metals & Ceramics
Metals possess:
• Good electrical & thermal conductivity, low hardness,
machinability, damage tolerance & thermal shock resistance
Ceramics possess:
• High-T strength, high elastic moduli,
oxidation & corrosion resistance.
 MAX materials possess both attributes - Exciting !!!!
So MAX materials are exciting new class of materials which
bridge the Gap between Metals & Ceramics
8-10 March 2018 BPS Conference-2018 5
8-10 March 2018 BPS Conference-2018 6
Properties Ceramic Metal MAX Phase Materials
Hardness H+ L G
Elastic Moduli H+ G G
High-T strength G L G
Thermal Expansion L G G
Ductility L G G
Oxidation resistance H L G-H
Corrosion resistance G-H L G
Resistance to wear G L G
Electrical Conductivity L- G G
Thermal Conductivity L- G G
Possess both attributes
(combine both Ceramic &
Metal properties)
Soft & machinable, yet
also heat-tolerant,
strong & lightweight
Major Challenges in Engineering & MAX
Materials
We need versatile materials for developing technologies.: Durable & high
performance in extreme environments
Now
1. Simple Facts from Thermodynamics!
 Efficiency of any fuel-burning engine: e ∝ Toperating
 Raise engine temp. by 1 oC  Fuel savings of the world’s jet alone worth ~
$1 b/year.
 Similar strategy to increase vehicle efficiency by 1 km/litre would save ~ 1 m
barrels of oil a day.
 A jet engine made from a material 50% lighter in weight & able to run 200 to
300 degrees hotter would have a staggering economic impact.
8-10 March 2018 BPS Conference-2018 7
2. Today's jet engines are not running hotter
for a simple reason :
• No material exists that can take that kind of heat
while spinning furiously.
The same goes for the internal-combustion engine;
if a car engine could be built with a temp-tolerant
material, its radiator, water pump & cooling water
could be thrown away.
• Such an efficient, lighter & higher-T engine would
squeeze more km from every litre of fuel.
8-10 March 2018 BPS Conference-2018 8
Contd.
Contd.
• Stiff, lightweight, machinable, made from relatively
inexpensive raw materials, resistant to oxidation &
thermal shock, & capable of remaining strong up to
T > 1300 oC in air.
• An ideal high-performance structural material for,
say, jet engines would have all these qualities.
• MAX materials form such a new class of
solids – since these turn out to be
surprisingly soft & machinable, yet also heat-
tolerant, strong & lightweight.
8-10 March 2018 BPS Conference-2018 9
Materials in demanding applications not only must
retain their strength, but also need to resist oxidation:
8-10 March 2018 BPS Conference-2018 10
T (oC) at which material ruptures after 140 MPa of stress for 10,000 hrs
T
at
which
oxidation
penetrates
2.5
mm
in
10,000
hrs
Ti3SiC2 possesses both
OUR Research on MAX Phases at RU + IIUC
 Prediction of yet unobserved phases
- First-principles investigation + Gibbs energy
- Thermodynamic, Electronic & Optical properties
 Substitution – strengthening study:
- Ti2-xVxAlC , Ti2SixAl1-xC etc.
 Superconducting MAX Phases (Thermal + optical prop)
- Nb2SC, Nb2SnC, Nb2AsC, Nb2InC
- Ti2InC, Ti2InN
- Mo2GaC
8-10 March 2018 BPS Conference-2018 11
Publication on MAX Phases = 24
A K M A Islam et al.
Year No. Journals
2018 2 J. Alloys & Comp, Mater. Res Express
2017 6 J. Alloys & Comp, Phys. Stat. Solidi, Comp. Mater. Sci, Chin. Phys B
2016 5 J.Phys: CMP, Comp.Mat. Sci, Chin.Phys B, Phys.Stat.Solidi
2015 2 Int.J.Mod.Phys., J.Sci.Res
2014 1 Int. J.Mod.Phys.
2013 4 Comp.Mater.Sci, Cond.Matter Phys., Int. Comp.Mater. Phys.
2012
2011
3
1
Physica B:CondMatter, ISRN Cond. Matter Phys,
Physica B:Cond.Matter
8-10 March 2018 BPS Conference-2018 12
During Last 6 years (2011 - 2018 Feb)
Total Publication = 53, Publ. on MAX Phases only = 24
Prediction of Yet Unobserved New MAX Phases
8-10 March 2018
BPS Conference-2018
13
T = 0, P = 0 : ∆E > 0, unstable; ∆E< 0, stable
Finite T, Finite P : ∆G > 0, unstable; ∆G< 0, stable
Energy difference ∆G(T, p) between the energy of MAX &
that of the competing phases (thermodynamically favorable)
is calculated using:
G(T, p) = Etot + (EZPE – T Svib) + p V
Here G = Gibb’s free energy, Etot = Total E (from electronic structure
calc.) , 2nd term = ZPE, & 3rd term = vibrational entropic
Stability of a MAX phase can be studied by comparing total energy
Phase Competing phases ∆E= EMAX-ECP
(eV/f.u.)
Reported occurrence
Ti2SiC 4/9 Ti3SiC2 + 1/9 TiSi2 + 1/9 Ti5Si3C
Ti3SiC2, TiSi2, Ti5Si3
0.014
- 0.032
No
Ti3SiC2 9/5 TiC+ 1/5 TiSi2 + 1/5 Ti5Si3C - 0.202 Yes
Ti4SiC3 Ti3SiC2+ TiC
Ti3SiC2+ TiC
0.012
- 0.232
Yes≠
Ti5SiC4 Ti3SiC2 + 2 TiC
Ti3SiC2 + 2 TiC
0.043
0.37 ?
No
Ti5Si2C3 Ti3SiC2, TiSi2, Ti5Si3
3/2 Ti3SiC2+ 1/7 TiSi2 + 1/14 Ti5Si3
0.36 Intergrown phase (IP)
hybrid “523” and “725” MAX phases
Ti7Si2C5 Ti3SiC2, TiC
2 Ti3SiC2+ TiC
0.392 IP (2004), Yes (2011)
8-10 March 2018
BPS Conference-2018
14
T = 0, P = 0 : ∆E > 0, unstable; ∆E< 0, stable
Finite T, Finite P : ∆G > 0, unstable; ∆G< 0, stable
a. Substitution (solid solution) of MAX phases
b. Superconducting MAX phases
The following properties are studied
Thermodynamic properties
 T & P dependence of Debye temp.
 T dependence of Cp, Cp
 T and P dependence of thermal expansion
Elastic properties
 Cij, B, shear modulus G, Y, ν
 Vickers hardness, brittleness
Electronic properties
 Electronic band structure, Total & partial DOS, Phonon etc
Optical properties + Thermoelectric Properties
 Dielectric constants, Photoconductivity
 Reflectivity spectrum
8-10 March 2018 BPS Conference-2018 15
Solid solution -- strengthening study
8-10 March 2018 BPS Conference-2018 16
 Ti2AlC can be strengthened by substituting Ti with
V to form (Ti,V)2AlC solid solutions.
 V is smaller, & has 1 more valence electron than Ti
The weak interaction transition metal-Al bonds
are reinforced & strengthened.
 B, Vicker’s hardness & other aspects are also
studied.
New Solid Solution of MAX Phases
M. Naguiba, et al. Mater.Res.Lett. 2014 Vol. 2, No. 4, 233–240
• Previously unreported Al containing solid solution Mn+1AXn phases
have recently been synthesized.
(Ti0.5,V0.5)3AlC2, (Nb0.5,V0.5)2AlC,
(Nb0.5,V0.5)4AlC3 , (Nb0.8, Zr0.2)2AlC
• Rietveld analysis of powder X-ray diffraction patterns was used to
calculate the lattice parameters & phase fractions.
• Heating Ti, V, Al & C elemental powders—in the molar ratio of
1.5:1.5:1.3:2—to 1, 450 ◦C for 2 h in flowing argon, resulted in a
predominantly phase pure sample of (Ti0.5,V0.5)3AlC2
• The other compositions were not as phase pure & further work on
optimizing the processing parameters needs to be carried out if
phase purity is desired.
8-10 March 2018 BPS Conference-2018 17
Thermodynamic properties
8-10 March 2018 BPS Conference-2018 18
At low T up to ~10 oC, CP = gT + bT3
g and b are the coefficients of electronic & lattice heat capacities.
A plot of CP/T vs T2 should yield a straight line with slope b & intercept g.
l (e-ph coupling constant) is obtained via g = (1+l) kB
2 N(EF)/3.
Thermodynamic Properties – contd.
8-10 March 2018 BPS Conference-2018 19
Optical Properties
8-10 March 2018 BPS Conference-2018 20
(a) Real and (b) imaginary part of dielectric function, (c) real and (d) imaginary part of refractive index,
(e) absorption coefficients, (f) loss function, (g) reflectivity and (h) real part of photoconductivity
Superconductors Ti2InC and Nb2SC
8-10 March 2018 BPS Conference-2018 21
Total & partial DOS of Ti2InC
Band structure of Ti2InC
Can calc, el-phonon coupling constant
Energy (eV)
0 10 20 30 40 50 60
Loss
function
0
2
4
6
8
10
12
Absorption
0
100000
200000
300000
Reflectivity
0.0
0.2
0.4
0.6
0.8
Fig :Optical constants of Nb2SC : (a) Reflectivity, (b) Absorption, (c) Loss function
(c)
(b)
(a)
Optical constants of Nb2SC (Tc = 5 K)
(Tc = 3.1 K)
Energy (eV)
0 10 20 30 40 50 60
Dielectric
function
-10
0
10
20
30
40
50
60
Real
Imaginary
Rrfractive
index
0
2
4
6
8
Conductivity
-4
-2
0
2
4
6
8
Real
Imaginary
EF
EF
Imaginary
Real
Fig : Optical constants of Nb2SC :(a) Conductivity, (b) Refractive index, (c) Diel
Outlook
Finally, the question: to what extent can the
properties of the MAX phases be tuned?
• Future research direction would be systematic exptl. studies of
MAX phase solid solutions to elucidate the role of chemistry on
phase stability and properties.
• To engineer the band structure by appropriate dopants, so
as to achieve desired properties (shifting Fermi level to tune
material from metal to semiconductor in a controlled manner).
• Combinatorial thin-film materials synthesis will be useful to
identify MAX phase solid solutions with attractive, and quite
possibly novel, properties.
8-10 March 2018 BPS Conference-2018 22
WONDER MATERIALS - Major Breakthrough in
Materials Science
 Graphene was the first
2D wonder material
Discovery: 2004
 Isolated at Manchester Univ - Nobel
Prize in Physics 2010
 A Geim & K Novoselov for ground-
breaking expts regarding 2D graphene
 Derived from parent 3D MAX phases
 “MXenes” are produced by etching
A-atom layer from MAX phases
 MXenes adopt 3 structures, as
inherited from the parent MAX
phases: M2X, M3X2, & M4X3
8-10 March 2018 BPS Conference-2018 23
Surface of a sheet of paper is two-dimensional
- can exist as 3, 5, or 7 atomic layers
Any shape that only has a surface area is a 2D
shape while shapes with volume are 3D shape
 Now MXene – New 2D
wonder material
Discovery 2011
MXenes – New 2D Wonder Materials
8-10 March 2018 BPS Conference-2018 24
MXenes, 2D materials, are derived from parent 3D MAX phases.
[
 “MXenes” are produced by etching A-atom layer from MAX
phases -- “ene” is affixed to emphasize their similarity to
Graphene
 MXenes adopt 3 structures, as inherited from the parent MAX
phases: M2X, M3X2, & M4X3
These 2D sheets/structures MXenes possess greatly different
properties – behavior typical of 2D Graphene materials.
Discovery
8-10 March 2018 BPS Conference-2018 25
Synthesis of Mxene
from MAX Phase
Solution approach to
Ti3AlC2 Exfoliation &
Dispersion
Etching process: simply immerse
MAX phase in hydrofluoric acid at
room-T.
Sonication
Exfoliate: Wash & Shed
flakes from surface
structures
Intercalation : Insertion of
a molecule (or ion) into
compounds with layered
structures
Apply sound energy
to agitate particles
MXene singled out
8-10 March 2018 BPS Conference-2018 26
HF-etching of Ti3AlC2
Scanning electron micrograph of
Exfoliated MXene nanosheets.
(mage: B Anasori, Drexel Univ)
Magnification = 20,000
split into thin flakes
Exfoliate: wash to get rid of flakes
Singled out:
Researchers have also figured out how to break layers
of MXenes, which are typically stacked like Pringles
potato chips, apart. So far, they’ve made MXene paper,
& are studying what is a single MXene layer can do.
Singled out
Intercalation is the insertion of a
molecule (or ion) into compounds
with layered structures
8-10 March 2018 BPS Conference-2018 27
DFT calculations showed that MXenes’ band gap can be tuned by changing the surface
termination, e.g. bare MXene is metallic conductors, while OH or F terminated are semiconductors with
small band gap.
Why's MXene good, then?
8-10 March 2018 BPS Conference-2018 28
3 main properties of MXene that should catch our eyes are:
1. It's hydrophilic. That means, unlike graphene, it loves water. And that's good
news.
2. It's very malleable. Can mold it into complicated forms, or roll or press it very
flat – both of which are potentially very handy for a material with conductivity.
3. The material has a very healthy capacitance of 900 F/cm3 – performance will
improve further. MXene lost no capacitance after >10,000 charge cycles.
This clay-like material, made
from etched MXene and
water, is not only easier and
safer to produce than current
electrode material, it’s also
has twice the capacitance!
Applications
• Electrical energy storage
Pseudocapacitors, Li-ion batteries, Hybrid devices
• Composite Materials
Conductive, high-strength, low-permeability polymers,
high strength & high toughness ceramic-metal composites
• Sensors – e.g. electrochemiluminescent sensor (2018)
• 2D and flexible electronics
• Spintronic Devices - 2D information superhighway
• 2D MXenes make photonic diodes (18 Jan 2018)
• MXenes can contain 'Electromagnetic Pollution‘
Buzzing sound/em noise, caused by radio waves, can originate from anything that
creates, carries or uses an electric current, including TV & internet cables, cell
phones, tablets & laptops.
• Use in Cell Phones that Charge in Seconds (15 Aug 2017)
https://phys.org/news/2016-09-electromagnetic-pollution-mxene-mobile-
devices.html#jCp
8-10 March 2018 BPS Conference-2018 29
MXene: A Breakthrough for Battery Charging?
July 30, 2017 by Sarah Chan
• No one enjoys waiting for their
phone to charge — but using a phone
with low battery can be even more
stressful. Fortunately, researchers
from Drexel University have
developed a new battery electrode
design that has the potential to
eliminate both of those problems.
They recently published their work in
the journal Nature Energy.
• The team, led by Dr. Yury Gogotsi,
created the new electrode design
from a highly conductive, 2-D
MXene.
What sets MXene apart from
traditional battery designs is its
ability to open up more paths for
ions to move quickly throughout the
material.
8-10 March 2018 BPS Conference-2018 30
https://i1.wp.com/media.giphy.com/media/xTiTnGs6ugGmS0tKC
Y/giphy.gif?w=1023&ssl=1
giphy.gif
8-10 March 2018 BPS Conference-2018 31
Ternary ceramics turn out to be surprisingly soft & machinable,
yet also heat-tolerant, strong & lightweight
 It’s hard to guess what the next couple of years
will bring to this new area of materials science.
But it’s clear that this is only the beginning.
Thank you

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AI-Invited-BPS Conf-8 March 2018.pdf

  • 1. Remarkable 3D MAX Phases & 2D Wonder Materials MXenes A.K.M. A. Islam Professor of Physics (Retd.), Rajshahi University 8-10 March 2018 BPS Conference-2018 1
  • 2. Outline  3D MAX Phase Materials (Nanolaminate): - Exciting new class of materials – Why ? - MAX phases: Bridging the gap between metals & ceramics - Applications  Our Research on MAX Phases  - Prediction of yet unobserved phases - Substitution – strengthening study: (Ti, V)2AlC2 etc. - Superconducting MAX phases  2D MXenes derived from 3D MAX Phases - Stories of new wonder materials 8-10 March 2018 BPS Conference-2018 2 Any shape that only has a surface area is a 2-D shape while shapes with volume are 3-D shapes. Lab: A K M A Islam Out of 91
  • 3. 3D MAX Phase Formula: Mn+1AXn – M is an early transition metal – A is an A-group element – X is either C or N 8-10 March 2018 BPS Conference-2018 3 Now > 70 phases-- most discovered & produced in powder form in the 60’s by H. Nowotny & coworkers. First fabricated in bulk & characterized (Dr. Barsoum Group at Drexel University, USA) MAX Materials Ti2InN Reactive hot-pressing of a ZrH2, Al & C powder mixture MAX Zr2AlC
  • 4. Exciting MAX Phases 8-10 March 2018 BPS Conference-2018 4 The term “MAX phases” was coined in the late 1990s. Renewed interest in MAX Phases after Barsoum & El-Raghy’s report in 1996 on the synthesis of phase-pure bulk T3SiC2 samples & their unusual combination of properties. Since then, Research on the MAX phases has exploded. According to ISI, to date > 1,200 papers have been published on one MAX phase alone, T3SiC2, with roughly half of those published in the past 6 years.
  • 5. Exciting MAX: Bridging the Gap between Metals & Ceramics Metals possess: • Good electrical & thermal conductivity, low hardness, machinability, damage tolerance & thermal shock resistance Ceramics possess: • High-T strength, high elastic moduli, oxidation & corrosion resistance.  MAX materials possess both attributes - Exciting !!!! So MAX materials are exciting new class of materials which bridge the Gap between Metals & Ceramics 8-10 March 2018 BPS Conference-2018 5
  • 6. 8-10 March 2018 BPS Conference-2018 6 Properties Ceramic Metal MAX Phase Materials Hardness H+ L G Elastic Moduli H+ G G High-T strength G L G Thermal Expansion L G G Ductility L G G Oxidation resistance H L G-H Corrosion resistance G-H L G Resistance to wear G L G Electrical Conductivity L- G G Thermal Conductivity L- G G Possess both attributes (combine both Ceramic & Metal properties) Soft & machinable, yet also heat-tolerant, strong & lightweight
  • 7. Major Challenges in Engineering & MAX Materials We need versatile materials for developing technologies.: Durable & high performance in extreme environments Now 1. Simple Facts from Thermodynamics!  Efficiency of any fuel-burning engine: e ∝ Toperating  Raise engine temp. by 1 oC  Fuel savings of the world’s jet alone worth ~ $1 b/year.  Similar strategy to increase vehicle efficiency by 1 km/litre would save ~ 1 m barrels of oil a day.  A jet engine made from a material 50% lighter in weight & able to run 200 to 300 degrees hotter would have a staggering economic impact. 8-10 March 2018 BPS Conference-2018 7
  • 8. 2. Today's jet engines are not running hotter for a simple reason : • No material exists that can take that kind of heat while spinning furiously. The same goes for the internal-combustion engine; if a car engine could be built with a temp-tolerant material, its radiator, water pump & cooling water could be thrown away. • Such an efficient, lighter & higher-T engine would squeeze more km from every litre of fuel. 8-10 March 2018 BPS Conference-2018 8 Contd.
  • 9. Contd. • Stiff, lightweight, machinable, made from relatively inexpensive raw materials, resistant to oxidation & thermal shock, & capable of remaining strong up to T > 1300 oC in air. • An ideal high-performance structural material for, say, jet engines would have all these qualities. • MAX materials form such a new class of solids – since these turn out to be surprisingly soft & machinable, yet also heat- tolerant, strong & lightweight. 8-10 March 2018 BPS Conference-2018 9
  • 10. Materials in demanding applications not only must retain their strength, but also need to resist oxidation: 8-10 March 2018 BPS Conference-2018 10 T (oC) at which material ruptures after 140 MPa of stress for 10,000 hrs T at which oxidation penetrates 2.5 mm in 10,000 hrs Ti3SiC2 possesses both
  • 11. OUR Research on MAX Phases at RU + IIUC  Prediction of yet unobserved phases - First-principles investigation + Gibbs energy - Thermodynamic, Electronic & Optical properties  Substitution – strengthening study: - Ti2-xVxAlC , Ti2SixAl1-xC etc.  Superconducting MAX Phases (Thermal + optical prop) - Nb2SC, Nb2SnC, Nb2AsC, Nb2InC - Ti2InC, Ti2InN - Mo2GaC 8-10 March 2018 BPS Conference-2018 11
  • 12. Publication on MAX Phases = 24 A K M A Islam et al. Year No. Journals 2018 2 J. Alloys & Comp, Mater. Res Express 2017 6 J. Alloys & Comp, Phys. Stat. Solidi, Comp. Mater. Sci, Chin. Phys B 2016 5 J.Phys: CMP, Comp.Mat. Sci, Chin.Phys B, Phys.Stat.Solidi 2015 2 Int.J.Mod.Phys., J.Sci.Res 2014 1 Int. J.Mod.Phys. 2013 4 Comp.Mater.Sci, Cond.Matter Phys., Int. Comp.Mater. Phys. 2012 2011 3 1 Physica B:CondMatter, ISRN Cond. Matter Phys, Physica B:Cond.Matter 8-10 March 2018 BPS Conference-2018 12 During Last 6 years (2011 - 2018 Feb) Total Publication = 53, Publ. on MAX Phases only = 24
  • 13. Prediction of Yet Unobserved New MAX Phases 8-10 March 2018 BPS Conference-2018 13 T = 0, P = 0 : ∆E > 0, unstable; ∆E< 0, stable Finite T, Finite P : ∆G > 0, unstable; ∆G< 0, stable Energy difference ∆G(T, p) between the energy of MAX & that of the competing phases (thermodynamically favorable) is calculated using: G(T, p) = Etot + (EZPE – T Svib) + p V Here G = Gibb’s free energy, Etot = Total E (from electronic structure calc.) , 2nd term = ZPE, & 3rd term = vibrational entropic Stability of a MAX phase can be studied by comparing total energy
  • 14. Phase Competing phases ∆E= EMAX-ECP (eV/f.u.) Reported occurrence Ti2SiC 4/9 Ti3SiC2 + 1/9 TiSi2 + 1/9 Ti5Si3C Ti3SiC2, TiSi2, Ti5Si3 0.014 - 0.032 No Ti3SiC2 9/5 TiC+ 1/5 TiSi2 + 1/5 Ti5Si3C - 0.202 Yes Ti4SiC3 Ti3SiC2+ TiC Ti3SiC2+ TiC 0.012 - 0.232 Yes≠ Ti5SiC4 Ti3SiC2 + 2 TiC Ti3SiC2 + 2 TiC 0.043 0.37 ? No Ti5Si2C3 Ti3SiC2, TiSi2, Ti5Si3 3/2 Ti3SiC2+ 1/7 TiSi2 + 1/14 Ti5Si3 0.36 Intergrown phase (IP) hybrid “523” and “725” MAX phases Ti7Si2C5 Ti3SiC2, TiC 2 Ti3SiC2+ TiC 0.392 IP (2004), Yes (2011) 8-10 March 2018 BPS Conference-2018 14 T = 0, P = 0 : ∆E > 0, unstable; ∆E< 0, stable Finite T, Finite P : ∆G > 0, unstable; ∆G< 0, stable
  • 15. a. Substitution (solid solution) of MAX phases b. Superconducting MAX phases The following properties are studied Thermodynamic properties  T & P dependence of Debye temp.  T dependence of Cp, Cp  T and P dependence of thermal expansion Elastic properties  Cij, B, shear modulus G, Y, ν  Vickers hardness, brittleness Electronic properties  Electronic band structure, Total & partial DOS, Phonon etc Optical properties + Thermoelectric Properties  Dielectric constants, Photoconductivity  Reflectivity spectrum 8-10 March 2018 BPS Conference-2018 15
  • 16. Solid solution -- strengthening study 8-10 March 2018 BPS Conference-2018 16  Ti2AlC can be strengthened by substituting Ti with V to form (Ti,V)2AlC solid solutions.  V is smaller, & has 1 more valence electron than Ti The weak interaction transition metal-Al bonds are reinforced & strengthened.  B, Vicker’s hardness & other aspects are also studied.
  • 17. New Solid Solution of MAX Phases M. Naguiba, et al. Mater.Res.Lett. 2014 Vol. 2, No. 4, 233–240 • Previously unreported Al containing solid solution Mn+1AXn phases have recently been synthesized. (Ti0.5,V0.5)3AlC2, (Nb0.5,V0.5)2AlC, (Nb0.5,V0.5)4AlC3 , (Nb0.8, Zr0.2)2AlC • Rietveld analysis of powder X-ray diffraction patterns was used to calculate the lattice parameters & phase fractions. • Heating Ti, V, Al & C elemental powders—in the molar ratio of 1.5:1.5:1.3:2—to 1, 450 ◦C for 2 h in flowing argon, resulted in a predominantly phase pure sample of (Ti0.5,V0.5)3AlC2 • The other compositions were not as phase pure & further work on optimizing the processing parameters needs to be carried out if phase purity is desired. 8-10 March 2018 BPS Conference-2018 17
  • 18. Thermodynamic properties 8-10 March 2018 BPS Conference-2018 18 At low T up to ~10 oC, CP = gT + bT3 g and b are the coefficients of electronic & lattice heat capacities. A plot of CP/T vs T2 should yield a straight line with slope b & intercept g. l (e-ph coupling constant) is obtained via g = (1+l) kB 2 N(EF)/3.
  • 19. Thermodynamic Properties – contd. 8-10 March 2018 BPS Conference-2018 19
  • 20. Optical Properties 8-10 March 2018 BPS Conference-2018 20 (a) Real and (b) imaginary part of dielectric function, (c) real and (d) imaginary part of refractive index, (e) absorption coefficients, (f) loss function, (g) reflectivity and (h) real part of photoconductivity
  • 21. Superconductors Ti2InC and Nb2SC 8-10 March 2018 BPS Conference-2018 21 Total & partial DOS of Ti2InC Band structure of Ti2InC Can calc, el-phonon coupling constant Energy (eV) 0 10 20 30 40 50 60 Loss function 0 2 4 6 8 10 12 Absorption 0 100000 200000 300000 Reflectivity 0.0 0.2 0.4 0.6 0.8 Fig :Optical constants of Nb2SC : (a) Reflectivity, (b) Absorption, (c) Loss function (c) (b) (a) Optical constants of Nb2SC (Tc = 5 K) (Tc = 3.1 K) Energy (eV) 0 10 20 30 40 50 60 Dielectric function -10 0 10 20 30 40 50 60 Real Imaginary Rrfractive index 0 2 4 6 8 Conductivity -4 -2 0 2 4 6 8 Real Imaginary EF EF Imaginary Real Fig : Optical constants of Nb2SC :(a) Conductivity, (b) Refractive index, (c) Diel
  • 22. Outlook Finally, the question: to what extent can the properties of the MAX phases be tuned? • Future research direction would be systematic exptl. studies of MAX phase solid solutions to elucidate the role of chemistry on phase stability and properties. • To engineer the band structure by appropriate dopants, so as to achieve desired properties (shifting Fermi level to tune material from metal to semiconductor in a controlled manner). • Combinatorial thin-film materials synthesis will be useful to identify MAX phase solid solutions with attractive, and quite possibly novel, properties. 8-10 March 2018 BPS Conference-2018 22
  • 23. WONDER MATERIALS - Major Breakthrough in Materials Science  Graphene was the first 2D wonder material Discovery: 2004  Isolated at Manchester Univ - Nobel Prize in Physics 2010  A Geim & K Novoselov for ground- breaking expts regarding 2D graphene  Derived from parent 3D MAX phases  “MXenes” are produced by etching A-atom layer from MAX phases  MXenes adopt 3 structures, as inherited from the parent MAX phases: M2X, M3X2, & M4X3 8-10 March 2018 BPS Conference-2018 23 Surface of a sheet of paper is two-dimensional - can exist as 3, 5, or 7 atomic layers Any shape that only has a surface area is a 2D shape while shapes with volume are 3D shape  Now MXene – New 2D wonder material Discovery 2011
  • 24. MXenes – New 2D Wonder Materials 8-10 March 2018 BPS Conference-2018 24 MXenes, 2D materials, are derived from parent 3D MAX phases. [  “MXenes” are produced by etching A-atom layer from MAX phases -- “ene” is affixed to emphasize their similarity to Graphene  MXenes adopt 3 structures, as inherited from the parent MAX phases: M2X, M3X2, & M4X3 These 2D sheets/structures MXenes possess greatly different properties – behavior typical of 2D Graphene materials. Discovery
  • 25. 8-10 March 2018 BPS Conference-2018 25 Synthesis of Mxene from MAX Phase Solution approach to Ti3AlC2 Exfoliation & Dispersion Etching process: simply immerse MAX phase in hydrofluoric acid at room-T. Sonication Exfoliate: Wash & Shed flakes from surface structures Intercalation : Insertion of a molecule (or ion) into compounds with layered structures Apply sound energy to agitate particles
  • 26. MXene singled out 8-10 March 2018 BPS Conference-2018 26 HF-etching of Ti3AlC2 Scanning electron micrograph of Exfoliated MXene nanosheets. (mage: B Anasori, Drexel Univ) Magnification = 20,000 split into thin flakes Exfoliate: wash to get rid of flakes Singled out: Researchers have also figured out how to break layers of MXenes, which are typically stacked like Pringles potato chips, apart. So far, they’ve made MXene paper, & are studying what is a single MXene layer can do. Singled out Intercalation is the insertion of a molecule (or ion) into compounds with layered structures
  • 27. 8-10 March 2018 BPS Conference-2018 27 DFT calculations showed that MXenes’ band gap can be tuned by changing the surface termination, e.g. bare MXene is metallic conductors, while OH or F terminated are semiconductors with small band gap.
  • 28. Why's MXene good, then? 8-10 March 2018 BPS Conference-2018 28 3 main properties of MXene that should catch our eyes are: 1. It's hydrophilic. That means, unlike graphene, it loves water. And that's good news. 2. It's very malleable. Can mold it into complicated forms, or roll or press it very flat – both of which are potentially very handy for a material with conductivity. 3. The material has a very healthy capacitance of 900 F/cm3 – performance will improve further. MXene lost no capacitance after >10,000 charge cycles. This clay-like material, made from etched MXene and water, is not only easier and safer to produce than current electrode material, it’s also has twice the capacitance!
  • 29. Applications • Electrical energy storage Pseudocapacitors, Li-ion batteries, Hybrid devices • Composite Materials Conductive, high-strength, low-permeability polymers, high strength & high toughness ceramic-metal composites • Sensors – e.g. electrochemiluminescent sensor (2018) • 2D and flexible electronics • Spintronic Devices - 2D information superhighway • 2D MXenes make photonic diodes (18 Jan 2018) • MXenes can contain 'Electromagnetic Pollution‘ Buzzing sound/em noise, caused by radio waves, can originate from anything that creates, carries or uses an electric current, including TV & internet cables, cell phones, tablets & laptops. • Use in Cell Phones that Charge in Seconds (15 Aug 2017) https://phys.org/news/2016-09-electromagnetic-pollution-mxene-mobile- devices.html#jCp 8-10 March 2018 BPS Conference-2018 29
  • 30. MXene: A Breakthrough for Battery Charging? July 30, 2017 by Sarah Chan • No one enjoys waiting for their phone to charge — but using a phone with low battery can be even more stressful. Fortunately, researchers from Drexel University have developed a new battery electrode design that has the potential to eliminate both of those problems. They recently published their work in the journal Nature Energy. • The team, led by Dr. Yury Gogotsi, created the new electrode design from a highly conductive, 2-D MXene. What sets MXene apart from traditional battery designs is its ability to open up more paths for ions to move quickly throughout the material. 8-10 March 2018 BPS Conference-2018 30 https://i1.wp.com/media.giphy.com/media/xTiTnGs6ugGmS0tKC Y/giphy.gif?w=1023&ssl=1 giphy.gif
  • 31. 8-10 March 2018 BPS Conference-2018 31 Ternary ceramics turn out to be surprisingly soft & machinable, yet also heat-tolerant, strong & lightweight  It’s hard to guess what the next couple of years will bring to this new area of materials science. But it’s clear that this is only the beginning. Thank you