Nanostrukturphysik (Nanostructure Physics) · react to form a Solid-Electrolyte Interphase(SEI)...
Transcript of Nanostrukturphysik (Nanostructure Physics) · react to form a Solid-Electrolyte Interphase(SEI)...
Fachgebiet 3D-Nanostrukturierung, Institut für Physik
Contact: [email protected]; [email protected]
Office: Unterpoerlitzer Straße 38 (Heisenbergbau) (tel: 3748) http://www.tu-ilmenau.de/3dnanostrukturierung/
Vorlesung: Wedsnesday 9:00 – 10:30, C 108
Übung: Friday (G), 9:00 – 10:30, C 110
Prof. Yong Lei & Dr. Yang Xu
(a) (b2) (b1)
UTAM-prepared free-standing one-dimensional surface nanostructures on Si
substrates: Ni nanowire arrays (a) and carbon nanotube arrays (b).
Nanostrukturphysik (Nanostructure Physics)
• Class 1: a general introduction of fundamentals of nano-structured materials, and definition
• Class 2: research at 3D-Nanostructuring (01)
• Class 3: research at 3D-Nanostructuring (02)
• Class 4: graphene
• Class 5: 2D atomically thin nanosheets
• Class 6: optical properties of 1D nanostructures
• Class 7: carbon nanotubes
• Class 8: solar water splitting I: fundamentals
• Class 9: solar water splitting II: nanostructures for water splitting
• Class 10: Lithium-ion batteries: Si nanostructures
• Class 11: Sodium-ion batteries and other ion batteries
• Class 12: Solar cells
Energy storage devices:
-Batteries -Supercapacitors
Osaka et al. Journal of Power Sources, 1997, 68, 173.
More power required for short time in
200 m race.
Supercapacitors
Constant but less power required for
long time in Marathon race.
Batteries
Energy storage devices:
-Batteries -Supercapacitors
A perfect athlete?
Starting materials of commercial LIBs
• Anode: graphite (layered structure)
• Cathode: layered lithium metal oxides, e.g.
LiCoO2, LiNiO2….
• Both electrodes are layered structures, so Li-
ions can insert into/extract from the electrode
materials
• Separator: ionic conductive, not electric
conductive
• Electrolyte: non-aqueous organic, air sensitive,
moisture sensitive (glove box)
First discharge of a commercial LIB
In the first discharge, the carbonates (solvent of electrolyte)
react to form a Solid-Electrolyte Interphase(SEI) layer on the
graphite electrode.
Lithiation
Existing technology
• Carbon anode (theoretical capacity 372
mAh/g for graphite)
• Lithium metal oxide or phosphate cathode
(LiCoO2, LiMn2O4, LiFePO4, theoretical
capacity 140-170 mAh/g)
Reaching its limit in energy density (per
volume, Wh/L; or per weight, Wh/kg) and
specific energy (per weight, mAh/g).
Opportunities and challenges for Si
anodes
Highest gravimetric capacity (4200 mAh/g)
Highest volumetric capacity (9786 mAh/cm3 calculated based on the
initial volume of Si)
Relatively low discharge voltage (0.4 V averagely)
Second-most abundant element in the earth’s crust and
environmental benign
A large and mature infrastructure for processing Si in industry
• Rapid capacity fading
• Large initial irreversible capacity,
i.e., low first cycle Coulombic
Efficiency (CE)
• A single crystalline-to-amorphous
phase transformation during the
first lithiation (discharging)
• Remains amorphous afterwards
Large volume changes during Li insertion and extraction:
420% volume expansion
Si particle size: 10 μm
Fundamental materials challenges to
use Si as a viable battery electrode
• Material pulverization
(volume change 420%)
• Morphology and
volume change of the
whole Si electrode
(current collector)
• Solid-electrolyte
interphase (SEI)
Nanostructured Si anodes
• Solid Si nanostructures
• Si nanowires (NWs)
• Core/shell Si NWs
• Si nanoparticles
• Hollow Si nanostructures
• Hollow Si nanostructures with clamping
Solid Si nanostructures-core-shell Si NWs (avoid pulverization)
• The core material is structurally stable and electrically conducting
• The shell material is the active Si for storing Li
Core: crystalline
Shell: amorphous
Cutoff: 150 mV Cutoff: 10 mV
J. Phys. Chem. C 2009, 113, 11390.
90% @ 100th cycle
88% capacity retention @ 6000 cycles
1000 mAh/g @ 12C
Fast charging/discharging up to 20C
Nat. Nanotechnol. 2012, 7, 309.
74% capacity retention
@ 1000 cycles
2800 mAh/g @ C/10
High CE: 99.84%
After 800 cycles
Nano Lett. 2012, 12, 3315.
Sodium-ion batteries (SIBs)
• Abundant
• Similar electrochemistry to Li system
• High ion conductivity of Na+-based electrolyte
Johnson et al. Advanced Functional Materials, 2013, 23, 947.
Cost, carbonates
Cost, current collectors at the anode
Number of publications
related to SIBs
(2014: ~250; 2015.10: ~340)
Komaba et al. Chem. Rev. 2014, 114, 11636
Goodenough et al. J. Am. Chem. Soc. 2013, 135, 1167
Tarascon et al. Science 2011, 334, 928
Komaba et al. Phys. Chem. Chem. Phys. 2014, 16, 15007
SIBs: Competitive performance
but lower cost!
Our strategies for high-performance SIBs
Defects, molecular configurations,
composites
Highly ordered arrays, 3D porous
structure Xu Y., Zhou M., Lei Y., Advanced Energy Materials (invited review
and front cover), 6 (7), DOI: 10.1002/aenm.201502514, 2016.
Electrode design ‒ highly ordered arrays
Oriented and facile pathways for electrons and Na-ions
Void spaces for restraining structural deviation of the single unit
Strong attachment to the substrate protecting from mechanical and
electrical separation
Xu Y., Zhou M., Lei Y., Advanced Energy Materials (invited review
and front cover), 6 (7), DOI: 10.1002/aenm.201502514, 2016.
Sb Ni Ni-TiO2
L. Liang, Y. Lei, et al. Energy & Environmental Science, 2015, 8, 2954;
Y. Xu, Y. Lei, et al. Chemistry of Materials, 2015, 27, 4274.
Half-cell
Full-cell
Stable output voltage (0.5 V for
half-cell and 2.9 V for full-cell)
High reversible capacity (600
mAh/g) and areal capacity (200
μAh/cm2)
Excellent rate capability (up to
20 A/g for both half- and full-
cell)
High energy and power density
for full-cell
Highly ordered Sb nanorod arrays
L. Liang, Y. Lei, et al. Energy & Environmental Science, 2015, 8, 2954.
Hierarchical leaf-like Sb as high-rate SIB anode
L. Liang, Y. Lei,* et al. J. Mater. Chem. A 2017, 5, 1749.
Half-cell performance
L. Liang, Y. Lei,* et al. J. Mater. Chem. A 2017, 5, 1749.
589 mAh/g at 0.5 A/g @ 150 cycles
Hierarchy: electrode stability
Small domain: short diffusion distance
Conductive additive- and binder-free: no “dead” weight
This work
Full-cell performance
L. Liang, Y. Lei,* et al. J. Mater. Chem. A 2017, 5, 1749.
• Full-cell: Sb (anode)/Na2/3Ni1/3Mn2/3O2 (cathode) • Average output voltage: ~2.9 V • Capacity: full realization of half-cell capacity • Rate capability: as high as 10 A/g
Hierarchical Sb-Ni nanoarrays as high-rate SIB anodes
L. Liang, Y. Lei,* et al. Nano Res. 2017, DOI: 10.1007/s12274-017-1536-0.
Sb
Ni
Half-cell performance
L. Liang, Y. Lei,* et al. Nano Res. 2017, DOI: 10.1007/s12274-017-1536-0.
High percentage of pseudocapacitance shows that rate capability depends on surface-controlled process instead of diffusion-controlled process.
Full-cell performance
L. Liang, Y. Lei,* et al. Nano Res. 2017, DOI: 10.1007/s12274-017-1536-0.
Fast charging and discharging
Structural stability after 200 cycles.
95 mAh/g
35 s/charge or discharge
Y. Xu, Y. Lei, et al. Chemistry of Materials, 2015, 27, 4274.
One of the most downloaded papers
in June, 2015!
200 mAh/g @50 mA/g after 100 cycles
Highly ordered Ni-TiO2 core-shell
nanopillar arrays
Electrode design ‒ highly
ordered arrays
Electrode design ‒ 3D porous structure
Amorphous TiO2 inverse opal structure
One of the best rate capability of
TiO2-based anode so far
First realization of inverse opal
structure for SIBs
First correlation of surface ion availability with solvent
wettability for SIBs
M. Zhou, Y. Lei, et al. Nano Energy, 31, 514-524, 2017.
Material design‒defects
Utilizing oxygen vacancies in SIBs for the first time
Promoted by surface thin-layer coating
Boosting the long-term cycling capacity by 4 times
and rate capability by 10 times, comparing to the
counterpart sample without oxygen vacancies
284 mAh/g @50 mA/g, 100 cycles 174 mAh/g @ 1 A/g
Y. Xu, Y. Lei, et al. Angewandte Chemie International Edition, 2015, 54, 8768
Ultrathin Al2O3-coated MoO3-x nanosheets
Oxygen vacancies (OVs) to boost sodium-storage of amorphous SnO2 anode
Y. Xu, Y. Lei,* et al. Nano Energy 2017, 38, 304.
• Highly ordered Ni/amorphous SnO2 core/shell nanoarrays: no influence from binder and conductive additive
• Annealing in N2 atmosphere: creating OVs • Annealing in air: no OVs
Half-cell performance
• Enhanced capacity at low rates • Significantly improved rate capability • One of the best rate capabilities of SIB anodes without
conductive additive: ~200 mAh/g at 10 and 20 A/g
50 mA/g
Y. Xu, Y. Lei,* et al. Nano Energy 2017, 38, 304.
Function of OVs
Better linear relationship between log(CV peak current) and log(CV scan rate): less limitation by diffusion-controlled process of charges
Less increased impedance with changing the angular frequency: higher Na diffusion coefficient (DNa).
Y. Xu, Y. Lei,* et al. Nano Energy 2017, 38, 304.
Material design ‒ molecular configurations Extended π-conjugated system
C. Wang, Y. Lei, et al. Journal of the American Chemical Society, 2015, 137, 3124;
C. Wang, Y Lei, et al. Advanced Functional Materials, 26, 1777-1786, 2016.
Stable output voltage (discharge plateau)
High reversible capacity
Excellent fast-charge and -discharge ability (up to 10 A/g)
Long cycling life (400 cycles (SSDC) and 1500 cycles (DSR) @ 1 A/g)
Among the best performance of organic SIB materials when published
SSDC
DSR
Material design ‒ molecular configurations
Extended π-conjugated system
(Anode)
(Cathode)
SSDC
(sodium 4,4”-stilbene-dicarboxylate)
C. Wang, Y. Lei, et al. Journal of the American Chemical Society, 2015, 137, 3124;
C. Wang, Y Lei, et al. Advanced Functional Materials, 26, 1777-1786, 2016.
A selectively permeable membrane for enhancing cyclability of organic SIB electrode
C. Wang, Y. Lei,* et al. Adv. Mater. 2016, 28, 9182.
Separator with large hole size: more active material diffusing through, more dissolving
Separator with pin hole-free coating: less active material diffusing through, less dissolving
PT as model material: 5,7,12,14-pentacenetetrone
• Large size permitting ion diffusion • Severe dissolution
PEDOT:PSS complex coated glass fiber separator
• Na-ion conductive • Pin hole-free
Our response to the challenge: potassium-ion batteries (PIBs)
• High abundance of K
• Close electrochemical potential (standard electrode
potential) of K (-2.92 V) to Li (-3.04 V) (better than Na -2.72 V)
• Carbon anode + Prussian blue-based cathode
Our work is the first report that represents PIBs with competitive rate capability and cyclability to LIBs using a carbon material.
Potassium Prussian blue (KPB) nanoparticles as potassium-ion battery cathode
3D framework: open channels Large interstitial sites: > 3 Å
Crystal size: 20-30 nm Domain size: ~8 nm
K0.220Fe[Fe(CN)6]0.805⋅□0.195⋅4.01H2O Great cyclability: 73.2 mAh g-1@50 cycles
C. Zhang, Y. Xu, Y. Lei,* et al. “Potassium Prussian blue nanoparticles: a low-cost cathode material for potassium-ion batteries” Adv. Funct. Mater. (back cover), 27 (4), 1604307, 2017.
Half-cell: KPB//K Full-cell: KPB//Carbon
C. Zhang, Y. Xu, Y. Lei,* et al. “Potassium Prussian blue nanoparticles: a low-cost cathode material for potassium-ion batteries” Adv. Funct. Mater. (back cover), 27 (4), 1604307, 2017.
13.07.2017 Seite 48 http://www.tu-ilmenau.de/3d-nanostrukturierung/
Advantages: • Higher energy density than conventional capacitors;
• Higher power density than batteries;
• Very high charge and discharge rate;
• Long cycling stability.
More power required for short time in
200 m race.
P. Simon, Y. Gogotsi, Nature Materials, 2008, 7, 845.
Supercapacitors
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Principle of supercapacitors
Charge storage mechanism:
Double-layer capacitors: Ionic adsorption at the electrode/electrolyte interface.
Pseudocapacitors: Fast surface redox
reactions between electrode and electrolyte.
Prerequisites on electrode to achieve
high-performance supercapacitors:
Large specific surface area;
Low ionic/electronic transport resistance.
Template-directed 3D nanostructure arrays
with highly-ordered structure and large specific surface area are the promising building blocks for construct high-
performance supercapacitors.
13.07.2017 Seite 50
Conductive nanotube arrays for construction of supercapacitors
Large surface area for ion adsorption and surface redox reactions;
Highly-ordered porous structure to ensure good utilization of the active material and
a short ion diffusion pathway;
Conductive core to provide fast electron transport.
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AAO
ALD
Pt
Etching
Transfer
MnO2
L. Wen, Y. Lei, et al. Small, 2014, 10, 3162.
Pt@MnO2 core/shell nanotube arrays with enhanced supercapacitor
performance
13.07.2017 Seite 52
“It is the main objective of today’s research to improve the specific
energy of supercapacitors without sacrificing power and cycle life.”
Increase specific capacitance (C) New active electrode materials;
Fast electrode kinetics and efficient material utilization.
Increase potential window (V) Asymmetric device configuration.
Challenge - Increasing specific energy
13.07.2017 Seite 53
Asymmetric supercapacitors based on core/shell nanotube arrays
AAO
ALD of SnO2 in AAO
SnO2 nanotubes
MnO2 (or PPy) coated on SnO2 nanotubes
SnO2/PPy
SnO2/MnO2
Separator
F. Grote, Y. Lei, Nano Energy, 2014, 10, 63; & Journal of Power Sources, 2014, 256, 37.
13.07.2017 Seite 54
Asymmetric supercapacitors based on core/shell nanotube arrays
F. Grote, Y. Lei, Nano Energy, 2014, 10, 63; & Journal of Power Sources, 2014, 256, 37.
13.07.2017 Seite 55
A key point of nanostructures for supercapacitor applications
Mechanical stability of nanostructure arrays during
device assembling process.
Mass loading of active materials.
1. Thick-layer of active materials;
2. Increasing specific surface area of nanostructured electrode.
13.07.2017 Seite 56
AAO Nanowires/Nanotubes
H. Zhao, Y. Lei, et al. Advanced Materials, 2014, 26, 7654.
13.07.2017 Seite 57 http://www.tu-ilmenau.de/3d-nanostrukturierung/
Metallic nanopore arrays replicated from AAO
AAO
Ni nanopores
H. Zhao, Y. Lei, et al. Advanced Materials, 2014, 26, 7654.
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0 20 40 60 80 1000
100
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Sp
ec
ific
ca
pa
cit
an
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/g)
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%)
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ten
tia
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Ag
/Ag
Cl)
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2
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Supercapacitor performance of Ni nanopores coated with MnO2
H. Zhao, Y. Lei, et al. Advanced Materials, 2014, 26, 7654.
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Ultrahigh-rate cable-type micro-supercapacitors based on polarized
TiO2 nanotubes
Vellacheri R., Lei Y, et al., Advanced Materials Technologies, in press (DOI: 10.1002/admt.201600012), 2016.
13.07.2017 Seite 61
Device assemble of cable-type micro-supercapacitors based on
polarized TiO2 nanotubes
Unpublished results
Such cable-type micro-supercapacitor with ultrahigh scan rate (200 V/s) as well as
impressive areal capacitance (0.86 F/cm2) should be beneficial for developing next-
generation flexible and/ wearable electronic devices.
Vellacheri R., Lei Y, et al., Advanced Materials Technologies, in press (DOI: 10.1002/admt.201600012), 2016.
13.07.2017 Seite 62
Supercapacitors based on Graphene
Flexible supercapacitors based on self-
stacked rGO–Co(1-x)Nix(OH)2 nanosheets
with fast electrochromic properties.
Graphene based supercapacitors for
efficient energy storage under extreme
environmental temperatures
R. Vellacheri, Y. Lei, et al. Nano Energy, 2014, 8, 231. F. Grote, Y. Lei, et al. Small, 2015, 11, 4666.
13.07.2017 www.tu-ilmenau.de/nanostruk Page 63
Wen L.Y., Lei Y., et al., Small (invited review) (frontispiece cover), 11, 3408, 2015.
Wang Z.J., Lei Y., et al., Nano Energy (invited review), 19, 328, 2016.
Zhao H., Lei Y., et al. Nano Energy (invited review), 2015,13, 790.
Xu Y., Zhou M., Lei Y.,Advanced Energy Materials (invited review), 6 (7), DOI: 10.1002/aenm.201502514, 2016.
13.07.2017 www.tu-ilmenau.de/nanostruk Page 64
1. Lei Y.*, ‘Functional Nanostructuring for Efficient Energy Conversion and Storage’, Advanced Energy
Materials (Invited Editorial), 6 (23), 201600461, 2016.
2. Wen L.Y., Zhou M., Wang. C.L., Mi Y., Lei Y.*, ‘Nanoengineering energy conversion and storage
devices via atomic layer deposition’, Advanced Energy Materials, 6 (23), 201600468, 2016.
3. Zhou M., Xu Y., Xiang J.X., Wang C.L., Liang L.Y., Fang Y.G., Wen L.Y., Mi Y., Lei Y.*,
‘Understanding the orderliness of atomic arrangement towards enhanced sodium storage’, Advanced
Energy Materials, 6 (23), 201600448, 2016.
Special issue ‘Functional Nanostructuring for
Efficient Energy Conversion and Storage’,
Advanced Energy Materials (impact
factor 15.230), 6 (23), Dec 9th, 2016.
• Class 1: a general introduction of fundamentals of nano-structured materials, and definition
• Class 2: research at 3D-Nanostructuring (01)
• Class 3: research at 3D-Nanostructuring (02)
• Class 4: graphene
• Class 5: 2D atomically thin nanosheets
• Class 6: optical properties of 1D nanostructures
• Class 7: carbon nanotubes
• Class 8: solar water splitting I: fundamentals
• Class 9: solar water splitting II: nanostructures for water splitting
• Class 10: Lithium-ion batteries: Si nanostructures
• Class 11: Sodium-ion batteries and other ion batteries
• Class 12: solar cells