jisoon ihm school of physics, seoul national university
DESCRIPTION
Electrical Switching in Carbon Nanotubes and Conformational Transformation of Chain Molecules. 2006. 8. 30. Jisoon Ihm School of Physics, Seoul National University. Collaborators. Sangbong Lee, Seungchul Kim, Byoung Wook Jeong (Seoul Nat’l Univ.) - PowerPoint PPT PresentationTRANSCRIPT
![Page 1: Jisoon Ihm School of Physics, Seoul National University](https://reader036.vdocuments.net/reader036/viewer/2022062723/56813b4d550346895da43eb8/html5/thumbnails/1.jpg)
Jisoon Ihm
School of Physics Seoul National University
Electrical Switching in Carbon Nanotubes and Conformational Transformation of C
hain Molecules
2006 8 30
Collaborators
bull Sangbong Lee Seungchul Kim Byoung Wook Jeong (Seoul Natrsquol Univ)
bull Young-Woo Son Marvin Cohen Steven Louie (Berkeley)
BasicsSubstitutional Impurity in Metallic Carbon Nanotubes
Boron or Nitrogen
Tube axis
Electronic Structure of Metallic Armchair Nanotube
Band structure of a (1010) single-wall nanotube ( LDA first-principles pseudopotential method )
VBM
CBM
Tube axis
Conductance with Boron Impurity
A
A
Similarity to acceptor states in semiconductors
HJ Choi et al PRL 84 2917(2000)
Conductance with Nitrogen Impurity
Similarity to donor states in semiconductors
D
D
I Electrical switching in metallic carbon nanotubes
( Y-W Son J Ihm etc Phys Rev Lett 95 216602(2005) )
bull Metallic and semiconducting carbon nanotubes are produced simultaneously
Selection Problem
bull Semiconducting nanotubes easy to change conductance using gate
bull Metallic nanotubes robust against impurities defects or external fffffffff fields (difficult to change conductance)
C
De
kke
r A
Z
ett
l1 Motivation
Is it possible to control the conductance of metallic single-wall carbon nanotubes
Interplay between defects and electric fields
electron flow
SB
L
ee
A
Z
ett
l1 Motivations ndash contrsquod
2 Calculational Method
SCattering-state appRoach for eLEctron Transport (SCARLET)
H J Choi et al PRB 59 2267(1999) and in preparation
Landauer formalism2
Nitrogen Boron
The electronic potential of N(B) is lowered Levels of quasibound states move down
The electronic potential of N(B) is raised Levels of quasibound states move up
3 B(N) doped (1010) SWNT
4 Switching in B-N codoped (1010) SWNT
N
B
bull Switching behavior offon ratio=607kΩ64kΩ~100
bull Maximum resistance depends on the relative position between N and B
bull Asymmetric resistance wrt the direction of Eext
∆H Eprop ext (diameter)2
5 Scaling for larger (nn) SWNT
6 Switching in (1010) SWNT with Vacancies
bull Four carbon atoms are removed (Strong repulsive potential)
bull Doubly degenerate quasibound states at fermi level
bull Switching behavior offon ratio=1200kΩ64kΩ ~200
bull Symmetric resistance wrt the direction of Eext
6 Switching in (1010) with Vacancies ndash contrsquod
Quasibound states move up or down depending on the direction of Eext
Summary
bull Conductance of metallic CNTs with impurities and applied electric fields is studied
bull With N and B impurity atoms on opposite sides asymmetric switching is possible using external fields
bull With a large vacancy complex symmetric switching is possible using external fields
II Conformational Transform of Azobenzene Molecules
( B-Y Choi et al Phys Rev Lett 96 156106(2006) )
Azobenzene (AB) C6H5-N=N-C6H5
Transformation between transAB and cisAB
(Voltage bias using STM)
Geometries of tAB
Geometries of cAB
Optimal geometry of tAB and cAB
STS for tAB and cAB
Disperse Orange 3 (NH2-C6H4-N=N-C6H4-NO2)
Flat geometry of cAB
Summary
bull Electrical pulse is found to induce molecular flip between trans and cis structures
Example of MATERIAL DESIGN totalreflection by three nitrogen impurities
Doubly degenerate impurity states cause perfect reflection at 06 eV
(Both even and odd states are fully reflected at same energy)
Importance of geometric symmetry (equilateral triangle)
Appendix
Difference between Eext and impurity potential U
Lippman-Schwinger formalism
Eigenstate |ψgt of Htot associated with the eigenstate |gt of H0 with the same energy E (with impurity potential U at site )
Projection on to the impurity |gt
where
Reflection for the specific state |gt
Total transmission
Resonance condition
With applied electric fields
Suppose ∆H at site α is ∆E
In other words is G0(αE) shifted by ∆E
G0 projected at site
Effect of Eext Greenrsquos function itself changes
(1010) SWNT with single attractive impurity of U=-5|t|
(1010) SWNT with a single attractive impurity of U=-5|t| while changing Eext
EF
(1010) SWNT with NO Eext while changing the strength of the attractive potential U
Changing Eext is different from changing U
SAMSUNG SDI FED ndash 2005 -
Picture1
Picture
2
Picture3
Picture
4
Power consumption of SED LCD PDP (36in)
SED
LCD
PDP
Canon-Toshiba SED at CEATEC2004
- Slide 1
- Slide 2
- Slide 3
- Slide 4
- Slide 5
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Collaborators
bull Sangbong Lee Seungchul Kim Byoung Wook Jeong (Seoul Natrsquol Univ)
bull Young-Woo Son Marvin Cohen Steven Louie (Berkeley)
BasicsSubstitutional Impurity in Metallic Carbon Nanotubes
Boron or Nitrogen
Tube axis
Electronic Structure of Metallic Armchair Nanotube
Band structure of a (1010) single-wall nanotube ( LDA first-principles pseudopotential method )
VBM
CBM
Tube axis
Conductance with Boron Impurity
A
A
Similarity to acceptor states in semiconductors
HJ Choi et al PRL 84 2917(2000)
Conductance with Nitrogen Impurity
Similarity to donor states in semiconductors
D
D
I Electrical switching in metallic carbon nanotubes
( Y-W Son J Ihm etc Phys Rev Lett 95 216602(2005) )
bull Metallic and semiconducting carbon nanotubes are produced simultaneously
Selection Problem
bull Semiconducting nanotubes easy to change conductance using gate
bull Metallic nanotubes robust against impurities defects or external fffffffff fields (difficult to change conductance)
C
De
kke
r A
Z
ett
l1 Motivation
Is it possible to control the conductance of metallic single-wall carbon nanotubes
Interplay between defects and electric fields
electron flow
SB
L
ee
A
Z
ett
l1 Motivations ndash contrsquod
2 Calculational Method
SCattering-state appRoach for eLEctron Transport (SCARLET)
H J Choi et al PRB 59 2267(1999) and in preparation
Landauer formalism2
Nitrogen Boron
The electronic potential of N(B) is lowered Levels of quasibound states move down
The electronic potential of N(B) is raised Levels of quasibound states move up
3 B(N) doped (1010) SWNT
4 Switching in B-N codoped (1010) SWNT
N
B
bull Switching behavior offon ratio=607kΩ64kΩ~100
bull Maximum resistance depends on the relative position between N and B
bull Asymmetric resistance wrt the direction of Eext
∆H Eprop ext (diameter)2
5 Scaling for larger (nn) SWNT
6 Switching in (1010) SWNT with Vacancies
bull Four carbon atoms are removed (Strong repulsive potential)
bull Doubly degenerate quasibound states at fermi level
bull Switching behavior offon ratio=1200kΩ64kΩ ~200
bull Symmetric resistance wrt the direction of Eext
6 Switching in (1010) with Vacancies ndash contrsquod
Quasibound states move up or down depending on the direction of Eext
Summary
bull Conductance of metallic CNTs with impurities and applied electric fields is studied
bull With N and B impurity atoms on opposite sides asymmetric switching is possible using external fields
bull With a large vacancy complex symmetric switching is possible using external fields
II Conformational Transform of Azobenzene Molecules
( B-Y Choi et al Phys Rev Lett 96 156106(2006) )
Azobenzene (AB) C6H5-N=N-C6H5
Transformation between transAB and cisAB
(Voltage bias using STM)
Geometries of tAB
Geometries of cAB
Optimal geometry of tAB and cAB
STS for tAB and cAB
Disperse Orange 3 (NH2-C6H4-N=N-C6H4-NO2)
Flat geometry of cAB
Summary
bull Electrical pulse is found to induce molecular flip between trans and cis structures
Example of MATERIAL DESIGN totalreflection by three nitrogen impurities
Doubly degenerate impurity states cause perfect reflection at 06 eV
(Both even and odd states are fully reflected at same energy)
Importance of geometric symmetry (equilateral triangle)
Appendix
Difference between Eext and impurity potential U
Lippman-Schwinger formalism
Eigenstate |ψgt of Htot associated with the eigenstate |gt of H0 with the same energy E (with impurity potential U at site )
Projection on to the impurity |gt
where
Reflection for the specific state |gt
Total transmission
Resonance condition
With applied electric fields
Suppose ∆H at site α is ∆E
In other words is G0(αE) shifted by ∆E
G0 projected at site
Effect of Eext Greenrsquos function itself changes
(1010) SWNT with single attractive impurity of U=-5|t|
(1010) SWNT with a single attractive impurity of U=-5|t| while changing Eext
EF
(1010) SWNT with NO Eext while changing the strength of the attractive potential U
Changing Eext is different from changing U
SAMSUNG SDI FED ndash 2005 -
Picture1
Picture
2
Picture3
Picture
4
Power consumption of SED LCD PDP (36in)
SED
LCD
PDP
Canon-Toshiba SED at CEATEC2004
- Slide 1
- Slide 2
- Slide 3
- Slide 4
- Slide 5
- Slide 6
- Slide 7
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![Page 3: Jisoon Ihm School of Physics, Seoul National University](https://reader036.vdocuments.net/reader036/viewer/2022062723/56813b4d550346895da43eb8/html5/thumbnails/3.jpg)
BasicsSubstitutional Impurity in Metallic Carbon Nanotubes
Boron or Nitrogen
Tube axis
Electronic Structure of Metallic Armchair Nanotube
Band structure of a (1010) single-wall nanotube ( LDA first-principles pseudopotential method )
VBM
CBM
Tube axis
Conductance with Boron Impurity
A
A
Similarity to acceptor states in semiconductors
HJ Choi et al PRL 84 2917(2000)
Conductance with Nitrogen Impurity
Similarity to donor states in semiconductors
D
D
I Electrical switching in metallic carbon nanotubes
( Y-W Son J Ihm etc Phys Rev Lett 95 216602(2005) )
bull Metallic and semiconducting carbon nanotubes are produced simultaneously
Selection Problem
bull Semiconducting nanotubes easy to change conductance using gate
bull Metallic nanotubes robust against impurities defects or external fffffffff fields (difficult to change conductance)
C
De
kke
r A
Z
ett
l1 Motivation
Is it possible to control the conductance of metallic single-wall carbon nanotubes
Interplay between defects and electric fields
electron flow
SB
L
ee
A
Z
ett
l1 Motivations ndash contrsquod
2 Calculational Method
SCattering-state appRoach for eLEctron Transport (SCARLET)
H J Choi et al PRB 59 2267(1999) and in preparation
Landauer formalism2
Nitrogen Boron
The electronic potential of N(B) is lowered Levels of quasibound states move down
The electronic potential of N(B) is raised Levels of quasibound states move up
3 B(N) doped (1010) SWNT
4 Switching in B-N codoped (1010) SWNT
N
B
bull Switching behavior offon ratio=607kΩ64kΩ~100
bull Maximum resistance depends on the relative position between N and B
bull Asymmetric resistance wrt the direction of Eext
∆H Eprop ext (diameter)2
5 Scaling for larger (nn) SWNT
6 Switching in (1010) SWNT with Vacancies
bull Four carbon atoms are removed (Strong repulsive potential)
bull Doubly degenerate quasibound states at fermi level
bull Switching behavior offon ratio=1200kΩ64kΩ ~200
bull Symmetric resistance wrt the direction of Eext
6 Switching in (1010) with Vacancies ndash contrsquod
Quasibound states move up or down depending on the direction of Eext
Summary
bull Conductance of metallic CNTs with impurities and applied electric fields is studied
bull With N and B impurity atoms on opposite sides asymmetric switching is possible using external fields
bull With a large vacancy complex symmetric switching is possible using external fields
II Conformational Transform of Azobenzene Molecules
( B-Y Choi et al Phys Rev Lett 96 156106(2006) )
Azobenzene (AB) C6H5-N=N-C6H5
Transformation between transAB and cisAB
(Voltage bias using STM)
Geometries of tAB
Geometries of cAB
Optimal geometry of tAB and cAB
STS for tAB and cAB
Disperse Orange 3 (NH2-C6H4-N=N-C6H4-NO2)
Flat geometry of cAB
Summary
bull Electrical pulse is found to induce molecular flip between trans and cis structures
Example of MATERIAL DESIGN totalreflection by three nitrogen impurities
Doubly degenerate impurity states cause perfect reflection at 06 eV
(Both even and odd states are fully reflected at same energy)
Importance of geometric symmetry (equilateral triangle)
Appendix
Difference between Eext and impurity potential U
Lippman-Schwinger formalism
Eigenstate |ψgt of Htot associated with the eigenstate |gt of H0 with the same energy E (with impurity potential U at site )
Projection on to the impurity |gt
where
Reflection for the specific state |gt
Total transmission
Resonance condition
With applied electric fields
Suppose ∆H at site α is ∆E
In other words is G0(αE) shifted by ∆E
G0 projected at site
Effect of Eext Greenrsquos function itself changes
(1010) SWNT with single attractive impurity of U=-5|t|
(1010) SWNT with a single attractive impurity of U=-5|t| while changing Eext
EF
(1010) SWNT with NO Eext while changing the strength of the attractive potential U
Changing Eext is different from changing U
SAMSUNG SDI FED ndash 2005 -
Picture1
Picture
2
Picture3
Picture
4
Power consumption of SED LCD PDP (36in)
SED
LCD
PDP
Canon-Toshiba SED at CEATEC2004
- Slide 1
- Slide 2
- Slide 3
- Slide 4
- Slide 5
- Slide 6
- Slide 7
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![Page 4: Jisoon Ihm School of Physics, Seoul National University](https://reader036.vdocuments.net/reader036/viewer/2022062723/56813b4d550346895da43eb8/html5/thumbnails/4.jpg)
Electronic Structure of Metallic Armchair Nanotube
Band structure of a (1010) single-wall nanotube ( LDA first-principles pseudopotential method )
VBM
CBM
Tube axis
Conductance with Boron Impurity
A
A
Similarity to acceptor states in semiconductors
HJ Choi et al PRL 84 2917(2000)
Conductance with Nitrogen Impurity
Similarity to donor states in semiconductors
D
D
I Electrical switching in metallic carbon nanotubes
( Y-W Son J Ihm etc Phys Rev Lett 95 216602(2005) )
bull Metallic and semiconducting carbon nanotubes are produced simultaneously
Selection Problem
bull Semiconducting nanotubes easy to change conductance using gate
bull Metallic nanotubes robust against impurities defects or external fffffffff fields (difficult to change conductance)
C
De
kke
r A
Z
ett
l1 Motivation
Is it possible to control the conductance of metallic single-wall carbon nanotubes
Interplay between defects and electric fields
electron flow
SB
L
ee
A
Z
ett
l1 Motivations ndash contrsquod
2 Calculational Method
SCattering-state appRoach for eLEctron Transport (SCARLET)
H J Choi et al PRB 59 2267(1999) and in preparation
Landauer formalism2
Nitrogen Boron
The electronic potential of N(B) is lowered Levels of quasibound states move down
The electronic potential of N(B) is raised Levels of quasibound states move up
3 B(N) doped (1010) SWNT
4 Switching in B-N codoped (1010) SWNT
N
B
bull Switching behavior offon ratio=607kΩ64kΩ~100
bull Maximum resistance depends on the relative position between N and B
bull Asymmetric resistance wrt the direction of Eext
∆H Eprop ext (diameter)2
5 Scaling for larger (nn) SWNT
6 Switching in (1010) SWNT with Vacancies
bull Four carbon atoms are removed (Strong repulsive potential)
bull Doubly degenerate quasibound states at fermi level
bull Switching behavior offon ratio=1200kΩ64kΩ ~200
bull Symmetric resistance wrt the direction of Eext
6 Switching in (1010) with Vacancies ndash contrsquod
Quasibound states move up or down depending on the direction of Eext
Summary
bull Conductance of metallic CNTs with impurities and applied electric fields is studied
bull With N and B impurity atoms on opposite sides asymmetric switching is possible using external fields
bull With a large vacancy complex symmetric switching is possible using external fields
II Conformational Transform of Azobenzene Molecules
( B-Y Choi et al Phys Rev Lett 96 156106(2006) )
Azobenzene (AB) C6H5-N=N-C6H5
Transformation between transAB and cisAB
(Voltage bias using STM)
Geometries of tAB
Geometries of cAB
Optimal geometry of tAB and cAB
STS for tAB and cAB
Disperse Orange 3 (NH2-C6H4-N=N-C6H4-NO2)
Flat geometry of cAB
Summary
bull Electrical pulse is found to induce molecular flip between trans and cis structures
Example of MATERIAL DESIGN totalreflection by three nitrogen impurities
Doubly degenerate impurity states cause perfect reflection at 06 eV
(Both even and odd states are fully reflected at same energy)
Importance of geometric symmetry (equilateral triangle)
Appendix
Difference between Eext and impurity potential U
Lippman-Schwinger formalism
Eigenstate |ψgt of Htot associated with the eigenstate |gt of H0 with the same energy E (with impurity potential U at site )
Projection on to the impurity |gt
where
Reflection for the specific state |gt
Total transmission
Resonance condition
With applied electric fields
Suppose ∆H at site α is ∆E
In other words is G0(αE) shifted by ∆E
G0 projected at site
Effect of Eext Greenrsquos function itself changes
(1010) SWNT with single attractive impurity of U=-5|t|
(1010) SWNT with a single attractive impurity of U=-5|t| while changing Eext
EF
(1010) SWNT with NO Eext while changing the strength of the attractive potential U
Changing Eext is different from changing U
SAMSUNG SDI FED ndash 2005 -
Picture1
Picture
2
Picture3
Picture
4
Power consumption of SED LCD PDP (36in)
SED
LCD
PDP
Canon-Toshiba SED at CEATEC2004
- Slide 1
- Slide 2
- Slide 3
- Slide 4
- Slide 5
- Slide 6
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![Page 5: Jisoon Ihm School of Physics, Seoul National University](https://reader036.vdocuments.net/reader036/viewer/2022062723/56813b4d550346895da43eb8/html5/thumbnails/5.jpg)
VBM
CBM
Tube axis
Conductance with Boron Impurity
A
A
Similarity to acceptor states in semiconductors
HJ Choi et al PRL 84 2917(2000)
Conductance with Nitrogen Impurity
Similarity to donor states in semiconductors
D
D
I Electrical switching in metallic carbon nanotubes
( Y-W Son J Ihm etc Phys Rev Lett 95 216602(2005) )
bull Metallic and semiconducting carbon nanotubes are produced simultaneously
Selection Problem
bull Semiconducting nanotubes easy to change conductance using gate
bull Metallic nanotubes robust against impurities defects or external fffffffff fields (difficult to change conductance)
C
De
kke
r A
Z
ett
l1 Motivation
Is it possible to control the conductance of metallic single-wall carbon nanotubes
Interplay between defects and electric fields
electron flow
SB
L
ee
A
Z
ett
l1 Motivations ndash contrsquod
2 Calculational Method
SCattering-state appRoach for eLEctron Transport (SCARLET)
H J Choi et al PRB 59 2267(1999) and in preparation
Landauer formalism2
Nitrogen Boron
The electronic potential of N(B) is lowered Levels of quasibound states move down
The electronic potential of N(B) is raised Levels of quasibound states move up
3 B(N) doped (1010) SWNT
4 Switching in B-N codoped (1010) SWNT
N
B
bull Switching behavior offon ratio=607kΩ64kΩ~100
bull Maximum resistance depends on the relative position between N and B
bull Asymmetric resistance wrt the direction of Eext
∆H Eprop ext (diameter)2
5 Scaling for larger (nn) SWNT
6 Switching in (1010) SWNT with Vacancies
bull Four carbon atoms are removed (Strong repulsive potential)
bull Doubly degenerate quasibound states at fermi level
bull Switching behavior offon ratio=1200kΩ64kΩ ~200
bull Symmetric resistance wrt the direction of Eext
6 Switching in (1010) with Vacancies ndash contrsquod
Quasibound states move up or down depending on the direction of Eext
Summary
bull Conductance of metallic CNTs with impurities and applied electric fields is studied
bull With N and B impurity atoms on opposite sides asymmetric switching is possible using external fields
bull With a large vacancy complex symmetric switching is possible using external fields
II Conformational Transform of Azobenzene Molecules
( B-Y Choi et al Phys Rev Lett 96 156106(2006) )
Azobenzene (AB) C6H5-N=N-C6H5
Transformation between transAB and cisAB
(Voltage bias using STM)
Geometries of tAB
Geometries of cAB
Optimal geometry of tAB and cAB
STS for tAB and cAB
Disperse Orange 3 (NH2-C6H4-N=N-C6H4-NO2)
Flat geometry of cAB
Summary
bull Electrical pulse is found to induce molecular flip between trans and cis structures
Example of MATERIAL DESIGN totalreflection by three nitrogen impurities
Doubly degenerate impurity states cause perfect reflection at 06 eV
(Both even and odd states are fully reflected at same energy)
Importance of geometric symmetry (equilateral triangle)
Appendix
Difference between Eext and impurity potential U
Lippman-Schwinger formalism
Eigenstate |ψgt of Htot associated with the eigenstate |gt of H0 with the same energy E (with impurity potential U at site )
Projection on to the impurity |gt
where
Reflection for the specific state |gt
Total transmission
Resonance condition
With applied electric fields
Suppose ∆H at site α is ∆E
In other words is G0(αE) shifted by ∆E
G0 projected at site
Effect of Eext Greenrsquos function itself changes
(1010) SWNT with single attractive impurity of U=-5|t|
(1010) SWNT with a single attractive impurity of U=-5|t| while changing Eext
EF
(1010) SWNT with NO Eext while changing the strength of the attractive potential U
Changing Eext is different from changing U
SAMSUNG SDI FED ndash 2005 -
Picture1
Picture
2
Picture3
Picture
4
Power consumption of SED LCD PDP (36in)
SED
LCD
PDP
Canon-Toshiba SED at CEATEC2004
- Slide 1
- Slide 2
- Slide 3
- Slide 4
- Slide 5
- Slide 6
- Slide 7
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-
![Page 6: Jisoon Ihm School of Physics, Seoul National University](https://reader036.vdocuments.net/reader036/viewer/2022062723/56813b4d550346895da43eb8/html5/thumbnails/6.jpg)
Tube axis
Conductance with Boron Impurity
A
A
Similarity to acceptor states in semiconductors
HJ Choi et al PRL 84 2917(2000)
Conductance with Nitrogen Impurity
Similarity to donor states in semiconductors
D
D
I Electrical switching in metallic carbon nanotubes
( Y-W Son J Ihm etc Phys Rev Lett 95 216602(2005) )
bull Metallic and semiconducting carbon nanotubes are produced simultaneously
Selection Problem
bull Semiconducting nanotubes easy to change conductance using gate
bull Metallic nanotubes robust against impurities defects or external fffffffff fields (difficult to change conductance)
C
De
kke
r A
Z
ett
l1 Motivation
Is it possible to control the conductance of metallic single-wall carbon nanotubes
Interplay between defects and electric fields
electron flow
SB
L
ee
A
Z
ett
l1 Motivations ndash contrsquod
2 Calculational Method
SCattering-state appRoach for eLEctron Transport (SCARLET)
H J Choi et al PRB 59 2267(1999) and in preparation
Landauer formalism2
Nitrogen Boron
The electronic potential of N(B) is lowered Levels of quasibound states move down
The electronic potential of N(B) is raised Levels of quasibound states move up
3 B(N) doped (1010) SWNT
4 Switching in B-N codoped (1010) SWNT
N
B
bull Switching behavior offon ratio=607kΩ64kΩ~100
bull Maximum resistance depends on the relative position between N and B
bull Asymmetric resistance wrt the direction of Eext
∆H Eprop ext (diameter)2
5 Scaling for larger (nn) SWNT
6 Switching in (1010) SWNT with Vacancies
bull Four carbon atoms are removed (Strong repulsive potential)
bull Doubly degenerate quasibound states at fermi level
bull Switching behavior offon ratio=1200kΩ64kΩ ~200
bull Symmetric resistance wrt the direction of Eext
6 Switching in (1010) with Vacancies ndash contrsquod
Quasibound states move up or down depending on the direction of Eext
Summary
bull Conductance of metallic CNTs with impurities and applied electric fields is studied
bull With N and B impurity atoms on opposite sides asymmetric switching is possible using external fields
bull With a large vacancy complex symmetric switching is possible using external fields
II Conformational Transform of Azobenzene Molecules
( B-Y Choi et al Phys Rev Lett 96 156106(2006) )
Azobenzene (AB) C6H5-N=N-C6H5
Transformation between transAB and cisAB
(Voltage bias using STM)
Geometries of tAB
Geometries of cAB
Optimal geometry of tAB and cAB
STS for tAB and cAB
Disperse Orange 3 (NH2-C6H4-N=N-C6H4-NO2)
Flat geometry of cAB
Summary
bull Electrical pulse is found to induce molecular flip between trans and cis structures
Example of MATERIAL DESIGN totalreflection by three nitrogen impurities
Doubly degenerate impurity states cause perfect reflection at 06 eV
(Both even and odd states are fully reflected at same energy)
Importance of geometric symmetry (equilateral triangle)
Appendix
Difference between Eext and impurity potential U
Lippman-Schwinger formalism
Eigenstate |ψgt of Htot associated with the eigenstate |gt of H0 with the same energy E (with impurity potential U at site )
Projection on to the impurity |gt
where
Reflection for the specific state |gt
Total transmission
Resonance condition
With applied electric fields
Suppose ∆H at site α is ∆E
In other words is G0(αE) shifted by ∆E
G0 projected at site
Effect of Eext Greenrsquos function itself changes
(1010) SWNT with single attractive impurity of U=-5|t|
(1010) SWNT with a single attractive impurity of U=-5|t| while changing Eext
EF
(1010) SWNT with NO Eext while changing the strength of the attractive potential U
Changing Eext is different from changing U
SAMSUNG SDI FED ndash 2005 -
Picture1
Picture
2
Picture3
Picture
4
Power consumption of SED LCD PDP (36in)
SED
LCD
PDP
Canon-Toshiba SED at CEATEC2004
- Slide 1
- Slide 2
- Slide 3
- Slide 4
- Slide 5
- Slide 6
- Slide 7
- Slide 8
- Slide 9
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-
![Page 7: Jisoon Ihm School of Physics, Seoul National University](https://reader036.vdocuments.net/reader036/viewer/2022062723/56813b4d550346895da43eb8/html5/thumbnails/7.jpg)
Conductance with Boron Impurity
A
A
Similarity to acceptor states in semiconductors
HJ Choi et al PRL 84 2917(2000)
Conductance with Nitrogen Impurity
Similarity to donor states in semiconductors
D
D
I Electrical switching in metallic carbon nanotubes
( Y-W Son J Ihm etc Phys Rev Lett 95 216602(2005) )
bull Metallic and semiconducting carbon nanotubes are produced simultaneously
Selection Problem
bull Semiconducting nanotubes easy to change conductance using gate
bull Metallic nanotubes robust against impurities defects or external fffffffff fields (difficult to change conductance)
C
De
kke
r A
Z
ett
l1 Motivation
Is it possible to control the conductance of metallic single-wall carbon nanotubes
Interplay between defects and electric fields
electron flow
SB
L
ee
A
Z
ett
l1 Motivations ndash contrsquod
2 Calculational Method
SCattering-state appRoach for eLEctron Transport (SCARLET)
H J Choi et al PRB 59 2267(1999) and in preparation
Landauer formalism2
Nitrogen Boron
The electronic potential of N(B) is lowered Levels of quasibound states move down
The electronic potential of N(B) is raised Levels of quasibound states move up
3 B(N) doped (1010) SWNT
4 Switching in B-N codoped (1010) SWNT
N
B
bull Switching behavior offon ratio=607kΩ64kΩ~100
bull Maximum resistance depends on the relative position between N and B
bull Asymmetric resistance wrt the direction of Eext
∆H Eprop ext (diameter)2
5 Scaling for larger (nn) SWNT
6 Switching in (1010) SWNT with Vacancies
bull Four carbon atoms are removed (Strong repulsive potential)
bull Doubly degenerate quasibound states at fermi level
bull Switching behavior offon ratio=1200kΩ64kΩ ~200
bull Symmetric resistance wrt the direction of Eext
6 Switching in (1010) with Vacancies ndash contrsquod
Quasibound states move up or down depending on the direction of Eext
Summary
bull Conductance of metallic CNTs with impurities and applied electric fields is studied
bull With N and B impurity atoms on opposite sides asymmetric switching is possible using external fields
bull With a large vacancy complex symmetric switching is possible using external fields
II Conformational Transform of Azobenzene Molecules
( B-Y Choi et al Phys Rev Lett 96 156106(2006) )
Azobenzene (AB) C6H5-N=N-C6H5
Transformation between transAB and cisAB
(Voltage bias using STM)
Geometries of tAB
Geometries of cAB
Optimal geometry of tAB and cAB
STS for tAB and cAB
Disperse Orange 3 (NH2-C6H4-N=N-C6H4-NO2)
Flat geometry of cAB
Summary
bull Electrical pulse is found to induce molecular flip between trans and cis structures
Example of MATERIAL DESIGN totalreflection by three nitrogen impurities
Doubly degenerate impurity states cause perfect reflection at 06 eV
(Both even and odd states are fully reflected at same energy)
Importance of geometric symmetry (equilateral triangle)
Appendix
Difference between Eext and impurity potential U
Lippman-Schwinger formalism
Eigenstate |ψgt of Htot associated with the eigenstate |gt of H0 with the same energy E (with impurity potential U at site )
Projection on to the impurity |gt
where
Reflection for the specific state |gt
Total transmission
Resonance condition
With applied electric fields
Suppose ∆H at site α is ∆E
In other words is G0(αE) shifted by ∆E
G0 projected at site
Effect of Eext Greenrsquos function itself changes
(1010) SWNT with single attractive impurity of U=-5|t|
(1010) SWNT with a single attractive impurity of U=-5|t| while changing Eext
EF
(1010) SWNT with NO Eext while changing the strength of the attractive potential U
Changing Eext is different from changing U
SAMSUNG SDI FED ndash 2005 -
Picture1
Picture
2
Picture3
Picture
4
Power consumption of SED LCD PDP (36in)
SED
LCD
PDP
Canon-Toshiba SED at CEATEC2004
- Slide 1
- Slide 2
- Slide 3
- Slide 4
- Slide 5
- Slide 6
- Slide 7
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-
![Page 8: Jisoon Ihm School of Physics, Seoul National University](https://reader036.vdocuments.net/reader036/viewer/2022062723/56813b4d550346895da43eb8/html5/thumbnails/8.jpg)
Conductance with Nitrogen Impurity
Similarity to donor states in semiconductors
D
D
I Electrical switching in metallic carbon nanotubes
( Y-W Son J Ihm etc Phys Rev Lett 95 216602(2005) )
bull Metallic and semiconducting carbon nanotubes are produced simultaneously
Selection Problem
bull Semiconducting nanotubes easy to change conductance using gate
bull Metallic nanotubes robust against impurities defects or external fffffffff fields (difficult to change conductance)
C
De
kke
r A
Z
ett
l1 Motivation
Is it possible to control the conductance of metallic single-wall carbon nanotubes
Interplay between defects and electric fields
electron flow
SB
L
ee
A
Z
ett
l1 Motivations ndash contrsquod
2 Calculational Method
SCattering-state appRoach for eLEctron Transport (SCARLET)
H J Choi et al PRB 59 2267(1999) and in preparation
Landauer formalism2
Nitrogen Boron
The electronic potential of N(B) is lowered Levels of quasibound states move down
The electronic potential of N(B) is raised Levels of quasibound states move up
3 B(N) doped (1010) SWNT
4 Switching in B-N codoped (1010) SWNT
N
B
bull Switching behavior offon ratio=607kΩ64kΩ~100
bull Maximum resistance depends on the relative position between N and B
bull Asymmetric resistance wrt the direction of Eext
∆H Eprop ext (diameter)2
5 Scaling for larger (nn) SWNT
6 Switching in (1010) SWNT with Vacancies
bull Four carbon atoms are removed (Strong repulsive potential)
bull Doubly degenerate quasibound states at fermi level
bull Switching behavior offon ratio=1200kΩ64kΩ ~200
bull Symmetric resistance wrt the direction of Eext
6 Switching in (1010) with Vacancies ndash contrsquod
Quasibound states move up or down depending on the direction of Eext
Summary
bull Conductance of metallic CNTs with impurities and applied electric fields is studied
bull With N and B impurity atoms on opposite sides asymmetric switching is possible using external fields
bull With a large vacancy complex symmetric switching is possible using external fields
II Conformational Transform of Azobenzene Molecules
( B-Y Choi et al Phys Rev Lett 96 156106(2006) )
Azobenzene (AB) C6H5-N=N-C6H5
Transformation between transAB and cisAB
(Voltage bias using STM)
Geometries of tAB
Geometries of cAB
Optimal geometry of tAB and cAB
STS for tAB and cAB
Disperse Orange 3 (NH2-C6H4-N=N-C6H4-NO2)
Flat geometry of cAB
Summary
bull Electrical pulse is found to induce molecular flip between trans and cis structures
Example of MATERIAL DESIGN totalreflection by three nitrogen impurities
Doubly degenerate impurity states cause perfect reflection at 06 eV
(Both even and odd states are fully reflected at same energy)
Importance of geometric symmetry (equilateral triangle)
Appendix
Difference between Eext and impurity potential U
Lippman-Schwinger formalism
Eigenstate |ψgt of Htot associated with the eigenstate |gt of H0 with the same energy E (with impurity potential U at site )
Projection on to the impurity |gt
where
Reflection for the specific state |gt
Total transmission
Resonance condition
With applied electric fields
Suppose ∆H at site α is ∆E
In other words is G0(αE) shifted by ∆E
G0 projected at site
Effect of Eext Greenrsquos function itself changes
(1010) SWNT with single attractive impurity of U=-5|t|
(1010) SWNT with a single attractive impurity of U=-5|t| while changing Eext
EF
(1010) SWNT with NO Eext while changing the strength of the attractive potential U
Changing Eext is different from changing U
SAMSUNG SDI FED ndash 2005 -
Picture1
Picture
2
Picture3
Picture
4
Power consumption of SED LCD PDP (36in)
SED
LCD
PDP
Canon-Toshiba SED at CEATEC2004
- Slide 1
- Slide 2
- Slide 3
- Slide 4
- Slide 5
- Slide 6
- Slide 7
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-
![Page 9: Jisoon Ihm School of Physics, Seoul National University](https://reader036.vdocuments.net/reader036/viewer/2022062723/56813b4d550346895da43eb8/html5/thumbnails/9.jpg)
I Electrical switching in metallic carbon nanotubes
( Y-W Son J Ihm etc Phys Rev Lett 95 216602(2005) )
bull Metallic and semiconducting carbon nanotubes are produced simultaneously
Selection Problem
bull Semiconducting nanotubes easy to change conductance using gate
bull Metallic nanotubes robust against impurities defects or external fffffffff fields (difficult to change conductance)
C
De
kke
r A
Z
ett
l1 Motivation
Is it possible to control the conductance of metallic single-wall carbon nanotubes
Interplay between defects and electric fields
electron flow
SB
L
ee
A
Z
ett
l1 Motivations ndash contrsquod
2 Calculational Method
SCattering-state appRoach for eLEctron Transport (SCARLET)
H J Choi et al PRB 59 2267(1999) and in preparation
Landauer formalism2
Nitrogen Boron
The electronic potential of N(B) is lowered Levels of quasibound states move down
The electronic potential of N(B) is raised Levels of quasibound states move up
3 B(N) doped (1010) SWNT
4 Switching in B-N codoped (1010) SWNT
N
B
bull Switching behavior offon ratio=607kΩ64kΩ~100
bull Maximum resistance depends on the relative position between N and B
bull Asymmetric resistance wrt the direction of Eext
∆H Eprop ext (diameter)2
5 Scaling for larger (nn) SWNT
6 Switching in (1010) SWNT with Vacancies
bull Four carbon atoms are removed (Strong repulsive potential)
bull Doubly degenerate quasibound states at fermi level
bull Switching behavior offon ratio=1200kΩ64kΩ ~200
bull Symmetric resistance wrt the direction of Eext
6 Switching in (1010) with Vacancies ndash contrsquod
Quasibound states move up or down depending on the direction of Eext
Summary
bull Conductance of metallic CNTs with impurities and applied electric fields is studied
bull With N and B impurity atoms on opposite sides asymmetric switching is possible using external fields
bull With a large vacancy complex symmetric switching is possible using external fields
II Conformational Transform of Azobenzene Molecules
( B-Y Choi et al Phys Rev Lett 96 156106(2006) )
Azobenzene (AB) C6H5-N=N-C6H5
Transformation between transAB and cisAB
(Voltage bias using STM)
Geometries of tAB
Geometries of cAB
Optimal geometry of tAB and cAB
STS for tAB and cAB
Disperse Orange 3 (NH2-C6H4-N=N-C6H4-NO2)
Flat geometry of cAB
Summary
bull Electrical pulse is found to induce molecular flip between trans and cis structures
Example of MATERIAL DESIGN totalreflection by three nitrogen impurities
Doubly degenerate impurity states cause perfect reflection at 06 eV
(Both even and odd states are fully reflected at same energy)
Importance of geometric symmetry (equilateral triangle)
Appendix
Difference between Eext and impurity potential U
Lippman-Schwinger formalism
Eigenstate |ψgt of Htot associated with the eigenstate |gt of H0 with the same energy E (with impurity potential U at site )
Projection on to the impurity |gt
where
Reflection for the specific state |gt
Total transmission
Resonance condition
With applied electric fields
Suppose ∆H at site α is ∆E
In other words is G0(αE) shifted by ∆E
G0 projected at site
Effect of Eext Greenrsquos function itself changes
(1010) SWNT with single attractive impurity of U=-5|t|
(1010) SWNT with a single attractive impurity of U=-5|t| while changing Eext
EF
(1010) SWNT with NO Eext while changing the strength of the attractive potential U
Changing Eext is different from changing U
SAMSUNG SDI FED ndash 2005 -
Picture1
Picture
2
Picture3
Picture
4
Power consumption of SED LCD PDP (36in)
SED
LCD
PDP
Canon-Toshiba SED at CEATEC2004
- Slide 1
- Slide 2
- Slide 3
- Slide 4
- Slide 5
- Slide 6
- Slide 7
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-
![Page 10: Jisoon Ihm School of Physics, Seoul National University](https://reader036.vdocuments.net/reader036/viewer/2022062723/56813b4d550346895da43eb8/html5/thumbnails/10.jpg)
bull Metallic and semiconducting carbon nanotubes are produced simultaneously
Selection Problem
bull Semiconducting nanotubes easy to change conductance using gate
bull Metallic nanotubes robust against impurities defects or external fffffffff fields (difficult to change conductance)
C
De
kke
r A
Z
ett
l1 Motivation
Is it possible to control the conductance of metallic single-wall carbon nanotubes
Interplay between defects and electric fields
electron flow
SB
L
ee
A
Z
ett
l1 Motivations ndash contrsquod
2 Calculational Method
SCattering-state appRoach for eLEctron Transport (SCARLET)
H J Choi et al PRB 59 2267(1999) and in preparation
Landauer formalism2
Nitrogen Boron
The electronic potential of N(B) is lowered Levels of quasibound states move down
The electronic potential of N(B) is raised Levels of quasibound states move up
3 B(N) doped (1010) SWNT
4 Switching in B-N codoped (1010) SWNT
N
B
bull Switching behavior offon ratio=607kΩ64kΩ~100
bull Maximum resistance depends on the relative position between N and B
bull Asymmetric resistance wrt the direction of Eext
∆H Eprop ext (diameter)2
5 Scaling for larger (nn) SWNT
6 Switching in (1010) SWNT with Vacancies
bull Four carbon atoms are removed (Strong repulsive potential)
bull Doubly degenerate quasibound states at fermi level
bull Switching behavior offon ratio=1200kΩ64kΩ ~200
bull Symmetric resistance wrt the direction of Eext
6 Switching in (1010) with Vacancies ndash contrsquod
Quasibound states move up or down depending on the direction of Eext
Summary
bull Conductance of metallic CNTs with impurities and applied electric fields is studied
bull With N and B impurity atoms on opposite sides asymmetric switching is possible using external fields
bull With a large vacancy complex symmetric switching is possible using external fields
II Conformational Transform of Azobenzene Molecules
( B-Y Choi et al Phys Rev Lett 96 156106(2006) )
Azobenzene (AB) C6H5-N=N-C6H5
Transformation between transAB and cisAB
(Voltage bias using STM)
Geometries of tAB
Geometries of cAB
Optimal geometry of tAB and cAB
STS for tAB and cAB
Disperse Orange 3 (NH2-C6H4-N=N-C6H4-NO2)
Flat geometry of cAB
Summary
bull Electrical pulse is found to induce molecular flip between trans and cis structures
Example of MATERIAL DESIGN totalreflection by three nitrogen impurities
Doubly degenerate impurity states cause perfect reflection at 06 eV
(Both even and odd states are fully reflected at same energy)
Importance of geometric symmetry (equilateral triangle)
Appendix
Difference between Eext and impurity potential U
Lippman-Schwinger formalism
Eigenstate |ψgt of Htot associated with the eigenstate |gt of H0 with the same energy E (with impurity potential U at site )
Projection on to the impurity |gt
where
Reflection for the specific state |gt
Total transmission
Resonance condition
With applied electric fields
Suppose ∆H at site α is ∆E
In other words is G0(αE) shifted by ∆E
G0 projected at site
Effect of Eext Greenrsquos function itself changes
(1010) SWNT with single attractive impurity of U=-5|t|
(1010) SWNT with a single attractive impurity of U=-5|t| while changing Eext
EF
(1010) SWNT with NO Eext while changing the strength of the attractive potential U
Changing Eext is different from changing U
SAMSUNG SDI FED ndash 2005 -
Picture1
Picture
2
Picture3
Picture
4
Power consumption of SED LCD PDP (36in)
SED
LCD
PDP
Canon-Toshiba SED at CEATEC2004
- Slide 1
- Slide 2
- Slide 3
- Slide 4
- Slide 5
- Slide 6
- Slide 7
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-
![Page 11: Jisoon Ihm School of Physics, Seoul National University](https://reader036.vdocuments.net/reader036/viewer/2022062723/56813b4d550346895da43eb8/html5/thumbnails/11.jpg)
Is it possible to control the conductance of metallic single-wall carbon nanotubes
Interplay between defects and electric fields
electron flow
SB
L
ee
A
Z
ett
l1 Motivations ndash contrsquod
2 Calculational Method
SCattering-state appRoach for eLEctron Transport (SCARLET)
H J Choi et al PRB 59 2267(1999) and in preparation
Landauer formalism2
Nitrogen Boron
The electronic potential of N(B) is lowered Levels of quasibound states move down
The electronic potential of N(B) is raised Levels of quasibound states move up
3 B(N) doped (1010) SWNT
4 Switching in B-N codoped (1010) SWNT
N
B
bull Switching behavior offon ratio=607kΩ64kΩ~100
bull Maximum resistance depends on the relative position between N and B
bull Asymmetric resistance wrt the direction of Eext
∆H Eprop ext (diameter)2
5 Scaling for larger (nn) SWNT
6 Switching in (1010) SWNT with Vacancies
bull Four carbon atoms are removed (Strong repulsive potential)
bull Doubly degenerate quasibound states at fermi level
bull Switching behavior offon ratio=1200kΩ64kΩ ~200
bull Symmetric resistance wrt the direction of Eext
6 Switching in (1010) with Vacancies ndash contrsquod
Quasibound states move up or down depending on the direction of Eext
Summary
bull Conductance of metallic CNTs with impurities and applied electric fields is studied
bull With N and B impurity atoms on opposite sides asymmetric switching is possible using external fields
bull With a large vacancy complex symmetric switching is possible using external fields
II Conformational Transform of Azobenzene Molecules
( B-Y Choi et al Phys Rev Lett 96 156106(2006) )
Azobenzene (AB) C6H5-N=N-C6H5
Transformation between transAB and cisAB
(Voltage bias using STM)
Geometries of tAB
Geometries of cAB
Optimal geometry of tAB and cAB
STS for tAB and cAB
Disperse Orange 3 (NH2-C6H4-N=N-C6H4-NO2)
Flat geometry of cAB
Summary
bull Electrical pulse is found to induce molecular flip between trans and cis structures
Example of MATERIAL DESIGN totalreflection by three nitrogen impurities
Doubly degenerate impurity states cause perfect reflection at 06 eV
(Both even and odd states are fully reflected at same energy)
Importance of geometric symmetry (equilateral triangle)
Appendix
Difference between Eext and impurity potential U
Lippman-Schwinger formalism
Eigenstate |ψgt of Htot associated with the eigenstate |gt of H0 with the same energy E (with impurity potential U at site )
Projection on to the impurity |gt
where
Reflection for the specific state |gt
Total transmission
Resonance condition
With applied electric fields
Suppose ∆H at site α is ∆E
In other words is G0(αE) shifted by ∆E
G0 projected at site
Effect of Eext Greenrsquos function itself changes
(1010) SWNT with single attractive impurity of U=-5|t|
(1010) SWNT with a single attractive impurity of U=-5|t| while changing Eext
EF
(1010) SWNT with NO Eext while changing the strength of the attractive potential U
Changing Eext is different from changing U
SAMSUNG SDI FED ndash 2005 -
Picture1
Picture
2
Picture3
Picture
4
Power consumption of SED LCD PDP (36in)
SED
LCD
PDP
Canon-Toshiba SED at CEATEC2004
- Slide 1
- Slide 2
- Slide 3
- Slide 4
- Slide 5
- Slide 6
- Slide 7
- Slide 8
- Slide 9
- Slide 10
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-
![Page 12: Jisoon Ihm School of Physics, Seoul National University](https://reader036.vdocuments.net/reader036/viewer/2022062723/56813b4d550346895da43eb8/html5/thumbnails/12.jpg)
2 Calculational Method
SCattering-state appRoach for eLEctron Transport (SCARLET)
H J Choi et al PRB 59 2267(1999) and in preparation
Landauer formalism2
Nitrogen Boron
The electronic potential of N(B) is lowered Levels of quasibound states move down
The electronic potential of N(B) is raised Levels of quasibound states move up
3 B(N) doped (1010) SWNT
4 Switching in B-N codoped (1010) SWNT
N
B
bull Switching behavior offon ratio=607kΩ64kΩ~100
bull Maximum resistance depends on the relative position between N and B
bull Asymmetric resistance wrt the direction of Eext
∆H Eprop ext (diameter)2
5 Scaling for larger (nn) SWNT
6 Switching in (1010) SWNT with Vacancies
bull Four carbon atoms are removed (Strong repulsive potential)
bull Doubly degenerate quasibound states at fermi level
bull Switching behavior offon ratio=1200kΩ64kΩ ~200
bull Symmetric resistance wrt the direction of Eext
6 Switching in (1010) with Vacancies ndash contrsquod
Quasibound states move up or down depending on the direction of Eext
Summary
bull Conductance of metallic CNTs with impurities and applied electric fields is studied
bull With N and B impurity atoms on opposite sides asymmetric switching is possible using external fields
bull With a large vacancy complex symmetric switching is possible using external fields
II Conformational Transform of Azobenzene Molecules
( B-Y Choi et al Phys Rev Lett 96 156106(2006) )
Azobenzene (AB) C6H5-N=N-C6H5
Transformation between transAB and cisAB
(Voltage bias using STM)
Geometries of tAB
Geometries of cAB
Optimal geometry of tAB and cAB
STS for tAB and cAB
Disperse Orange 3 (NH2-C6H4-N=N-C6H4-NO2)
Flat geometry of cAB
Summary
bull Electrical pulse is found to induce molecular flip between trans and cis structures
Example of MATERIAL DESIGN totalreflection by three nitrogen impurities
Doubly degenerate impurity states cause perfect reflection at 06 eV
(Both even and odd states are fully reflected at same energy)
Importance of geometric symmetry (equilateral triangle)
Appendix
Difference between Eext and impurity potential U
Lippman-Schwinger formalism
Eigenstate |ψgt of Htot associated with the eigenstate |gt of H0 with the same energy E (with impurity potential U at site )
Projection on to the impurity |gt
where
Reflection for the specific state |gt
Total transmission
Resonance condition
With applied electric fields
Suppose ∆H at site α is ∆E
In other words is G0(αE) shifted by ∆E
G0 projected at site
Effect of Eext Greenrsquos function itself changes
(1010) SWNT with single attractive impurity of U=-5|t|
(1010) SWNT with a single attractive impurity of U=-5|t| while changing Eext
EF
(1010) SWNT with NO Eext while changing the strength of the attractive potential U
Changing Eext is different from changing U
SAMSUNG SDI FED ndash 2005 -
Picture1
Picture
2
Picture3
Picture
4
Power consumption of SED LCD PDP (36in)
SED
LCD
PDP
Canon-Toshiba SED at CEATEC2004
- Slide 1
- Slide 2
- Slide 3
- Slide 4
- Slide 5
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![Page 13: Jisoon Ihm School of Physics, Seoul National University](https://reader036.vdocuments.net/reader036/viewer/2022062723/56813b4d550346895da43eb8/html5/thumbnails/13.jpg)
Nitrogen Boron
The electronic potential of N(B) is lowered Levels of quasibound states move down
The electronic potential of N(B) is raised Levels of quasibound states move up
3 B(N) doped (1010) SWNT
4 Switching in B-N codoped (1010) SWNT
N
B
bull Switching behavior offon ratio=607kΩ64kΩ~100
bull Maximum resistance depends on the relative position between N and B
bull Asymmetric resistance wrt the direction of Eext
∆H Eprop ext (diameter)2
5 Scaling for larger (nn) SWNT
6 Switching in (1010) SWNT with Vacancies
bull Four carbon atoms are removed (Strong repulsive potential)
bull Doubly degenerate quasibound states at fermi level
bull Switching behavior offon ratio=1200kΩ64kΩ ~200
bull Symmetric resistance wrt the direction of Eext
6 Switching in (1010) with Vacancies ndash contrsquod
Quasibound states move up or down depending on the direction of Eext
Summary
bull Conductance of metallic CNTs with impurities and applied electric fields is studied
bull With N and B impurity atoms on opposite sides asymmetric switching is possible using external fields
bull With a large vacancy complex symmetric switching is possible using external fields
II Conformational Transform of Azobenzene Molecules
( B-Y Choi et al Phys Rev Lett 96 156106(2006) )
Azobenzene (AB) C6H5-N=N-C6H5
Transformation between transAB and cisAB
(Voltage bias using STM)
Geometries of tAB
Geometries of cAB
Optimal geometry of tAB and cAB
STS for tAB and cAB
Disperse Orange 3 (NH2-C6H4-N=N-C6H4-NO2)
Flat geometry of cAB
Summary
bull Electrical pulse is found to induce molecular flip between trans and cis structures
Example of MATERIAL DESIGN totalreflection by three nitrogen impurities
Doubly degenerate impurity states cause perfect reflection at 06 eV
(Both even and odd states are fully reflected at same energy)
Importance of geometric symmetry (equilateral triangle)
Appendix
Difference between Eext and impurity potential U
Lippman-Schwinger formalism
Eigenstate |ψgt of Htot associated with the eigenstate |gt of H0 with the same energy E (with impurity potential U at site )
Projection on to the impurity |gt
where
Reflection for the specific state |gt
Total transmission
Resonance condition
With applied electric fields
Suppose ∆H at site α is ∆E
In other words is G0(αE) shifted by ∆E
G0 projected at site
Effect of Eext Greenrsquos function itself changes
(1010) SWNT with single attractive impurity of U=-5|t|
(1010) SWNT with a single attractive impurity of U=-5|t| while changing Eext
EF
(1010) SWNT with NO Eext while changing the strength of the attractive potential U
Changing Eext is different from changing U
SAMSUNG SDI FED ndash 2005 -
Picture1
Picture
2
Picture3
Picture
4
Power consumption of SED LCD PDP (36in)
SED
LCD
PDP
Canon-Toshiba SED at CEATEC2004
- Slide 1
- Slide 2
- Slide 3
- Slide 4
- Slide 5
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-
![Page 14: Jisoon Ihm School of Physics, Seoul National University](https://reader036.vdocuments.net/reader036/viewer/2022062723/56813b4d550346895da43eb8/html5/thumbnails/14.jpg)
4 Switching in B-N codoped (1010) SWNT
N
B
bull Switching behavior offon ratio=607kΩ64kΩ~100
bull Maximum resistance depends on the relative position between N and B
bull Asymmetric resistance wrt the direction of Eext
∆H Eprop ext (diameter)2
5 Scaling for larger (nn) SWNT
6 Switching in (1010) SWNT with Vacancies
bull Four carbon atoms are removed (Strong repulsive potential)
bull Doubly degenerate quasibound states at fermi level
bull Switching behavior offon ratio=1200kΩ64kΩ ~200
bull Symmetric resistance wrt the direction of Eext
6 Switching in (1010) with Vacancies ndash contrsquod
Quasibound states move up or down depending on the direction of Eext
Summary
bull Conductance of metallic CNTs with impurities and applied electric fields is studied
bull With N and B impurity atoms on opposite sides asymmetric switching is possible using external fields
bull With a large vacancy complex symmetric switching is possible using external fields
II Conformational Transform of Azobenzene Molecules
( B-Y Choi et al Phys Rev Lett 96 156106(2006) )
Azobenzene (AB) C6H5-N=N-C6H5
Transformation between transAB and cisAB
(Voltage bias using STM)
Geometries of tAB
Geometries of cAB
Optimal geometry of tAB and cAB
STS for tAB and cAB
Disperse Orange 3 (NH2-C6H4-N=N-C6H4-NO2)
Flat geometry of cAB
Summary
bull Electrical pulse is found to induce molecular flip between trans and cis structures
Example of MATERIAL DESIGN totalreflection by three nitrogen impurities
Doubly degenerate impurity states cause perfect reflection at 06 eV
(Both even and odd states are fully reflected at same energy)
Importance of geometric symmetry (equilateral triangle)
Appendix
Difference between Eext and impurity potential U
Lippman-Schwinger formalism
Eigenstate |ψgt of Htot associated with the eigenstate |gt of H0 with the same energy E (with impurity potential U at site )
Projection on to the impurity |gt
where
Reflection for the specific state |gt
Total transmission
Resonance condition
With applied electric fields
Suppose ∆H at site α is ∆E
In other words is G0(αE) shifted by ∆E
G0 projected at site
Effect of Eext Greenrsquos function itself changes
(1010) SWNT with single attractive impurity of U=-5|t|
(1010) SWNT with a single attractive impurity of U=-5|t| while changing Eext
EF
(1010) SWNT with NO Eext while changing the strength of the attractive potential U
Changing Eext is different from changing U
SAMSUNG SDI FED ndash 2005 -
Picture1
Picture
2
Picture3
Picture
4
Power consumption of SED LCD PDP (36in)
SED
LCD
PDP
Canon-Toshiba SED at CEATEC2004
- Slide 1
- Slide 2
- Slide 3
- Slide 4
- Slide 5
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-
![Page 15: Jisoon Ihm School of Physics, Seoul National University](https://reader036.vdocuments.net/reader036/viewer/2022062723/56813b4d550346895da43eb8/html5/thumbnails/15.jpg)
∆H Eprop ext (diameter)2
5 Scaling for larger (nn) SWNT
6 Switching in (1010) SWNT with Vacancies
bull Four carbon atoms are removed (Strong repulsive potential)
bull Doubly degenerate quasibound states at fermi level
bull Switching behavior offon ratio=1200kΩ64kΩ ~200
bull Symmetric resistance wrt the direction of Eext
6 Switching in (1010) with Vacancies ndash contrsquod
Quasibound states move up or down depending on the direction of Eext
Summary
bull Conductance of metallic CNTs with impurities and applied electric fields is studied
bull With N and B impurity atoms on opposite sides asymmetric switching is possible using external fields
bull With a large vacancy complex symmetric switching is possible using external fields
II Conformational Transform of Azobenzene Molecules
( B-Y Choi et al Phys Rev Lett 96 156106(2006) )
Azobenzene (AB) C6H5-N=N-C6H5
Transformation between transAB and cisAB
(Voltage bias using STM)
Geometries of tAB
Geometries of cAB
Optimal geometry of tAB and cAB
STS for tAB and cAB
Disperse Orange 3 (NH2-C6H4-N=N-C6H4-NO2)
Flat geometry of cAB
Summary
bull Electrical pulse is found to induce molecular flip between trans and cis structures
Example of MATERIAL DESIGN totalreflection by three nitrogen impurities
Doubly degenerate impurity states cause perfect reflection at 06 eV
(Both even and odd states are fully reflected at same energy)
Importance of geometric symmetry (equilateral triangle)
Appendix
Difference between Eext and impurity potential U
Lippman-Schwinger formalism
Eigenstate |ψgt of Htot associated with the eigenstate |gt of H0 with the same energy E (with impurity potential U at site )
Projection on to the impurity |gt
where
Reflection for the specific state |gt
Total transmission
Resonance condition
With applied electric fields
Suppose ∆H at site α is ∆E
In other words is G0(αE) shifted by ∆E
G0 projected at site
Effect of Eext Greenrsquos function itself changes
(1010) SWNT with single attractive impurity of U=-5|t|
(1010) SWNT with a single attractive impurity of U=-5|t| while changing Eext
EF
(1010) SWNT with NO Eext while changing the strength of the attractive potential U
Changing Eext is different from changing U
SAMSUNG SDI FED ndash 2005 -
Picture1
Picture
2
Picture3
Picture
4
Power consumption of SED LCD PDP (36in)
SED
LCD
PDP
Canon-Toshiba SED at CEATEC2004
- Slide 1
- Slide 2
- Slide 3
- Slide 4
- Slide 5
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![Page 16: Jisoon Ihm School of Physics, Seoul National University](https://reader036.vdocuments.net/reader036/viewer/2022062723/56813b4d550346895da43eb8/html5/thumbnails/16.jpg)
6 Switching in (1010) SWNT with Vacancies
bull Four carbon atoms are removed (Strong repulsive potential)
bull Doubly degenerate quasibound states at fermi level
bull Switching behavior offon ratio=1200kΩ64kΩ ~200
bull Symmetric resistance wrt the direction of Eext
6 Switching in (1010) with Vacancies ndash contrsquod
Quasibound states move up or down depending on the direction of Eext
Summary
bull Conductance of metallic CNTs with impurities and applied electric fields is studied
bull With N and B impurity atoms on opposite sides asymmetric switching is possible using external fields
bull With a large vacancy complex symmetric switching is possible using external fields
II Conformational Transform of Azobenzene Molecules
( B-Y Choi et al Phys Rev Lett 96 156106(2006) )
Azobenzene (AB) C6H5-N=N-C6H5
Transformation between transAB and cisAB
(Voltage bias using STM)
Geometries of tAB
Geometries of cAB
Optimal geometry of tAB and cAB
STS for tAB and cAB
Disperse Orange 3 (NH2-C6H4-N=N-C6H4-NO2)
Flat geometry of cAB
Summary
bull Electrical pulse is found to induce molecular flip between trans and cis structures
Example of MATERIAL DESIGN totalreflection by three nitrogen impurities
Doubly degenerate impurity states cause perfect reflection at 06 eV
(Both even and odd states are fully reflected at same energy)
Importance of geometric symmetry (equilateral triangle)
Appendix
Difference between Eext and impurity potential U
Lippman-Schwinger formalism
Eigenstate |ψgt of Htot associated with the eigenstate |gt of H0 with the same energy E (with impurity potential U at site )
Projection on to the impurity |gt
where
Reflection for the specific state |gt
Total transmission
Resonance condition
With applied electric fields
Suppose ∆H at site α is ∆E
In other words is G0(αE) shifted by ∆E
G0 projected at site
Effect of Eext Greenrsquos function itself changes
(1010) SWNT with single attractive impurity of U=-5|t|
(1010) SWNT with a single attractive impurity of U=-5|t| while changing Eext
EF
(1010) SWNT with NO Eext while changing the strength of the attractive potential U
Changing Eext is different from changing U
SAMSUNG SDI FED ndash 2005 -
Picture1
Picture
2
Picture3
Picture
4
Power consumption of SED LCD PDP (36in)
SED
LCD
PDP
Canon-Toshiba SED at CEATEC2004
- Slide 1
- Slide 2
- Slide 3
- Slide 4
- Slide 5
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-
![Page 17: Jisoon Ihm School of Physics, Seoul National University](https://reader036.vdocuments.net/reader036/viewer/2022062723/56813b4d550346895da43eb8/html5/thumbnails/17.jpg)
6 Switching in (1010) with Vacancies ndash contrsquod
Quasibound states move up or down depending on the direction of Eext
Summary
bull Conductance of metallic CNTs with impurities and applied electric fields is studied
bull With N and B impurity atoms on opposite sides asymmetric switching is possible using external fields
bull With a large vacancy complex symmetric switching is possible using external fields
II Conformational Transform of Azobenzene Molecules
( B-Y Choi et al Phys Rev Lett 96 156106(2006) )
Azobenzene (AB) C6H5-N=N-C6H5
Transformation between transAB and cisAB
(Voltage bias using STM)
Geometries of tAB
Geometries of cAB
Optimal geometry of tAB and cAB
STS for tAB and cAB
Disperse Orange 3 (NH2-C6H4-N=N-C6H4-NO2)
Flat geometry of cAB
Summary
bull Electrical pulse is found to induce molecular flip between trans and cis structures
Example of MATERIAL DESIGN totalreflection by three nitrogen impurities
Doubly degenerate impurity states cause perfect reflection at 06 eV
(Both even and odd states are fully reflected at same energy)
Importance of geometric symmetry (equilateral triangle)
Appendix
Difference between Eext and impurity potential U
Lippman-Schwinger formalism
Eigenstate |ψgt of Htot associated with the eigenstate |gt of H0 with the same energy E (with impurity potential U at site )
Projection on to the impurity |gt
where
Reflection for the specific state |gt
Total transmission
Resonance condition
With applied electric fields
Suppose ∆H at site α is ∆E
In other words is G0(αE) shifted by ∆E
G0 projected at site
Effect of Eext Greenrsquos function itself changes
(1010) SWNT with single attractive impurity of U=-5|t|
(1010) SWNT with a single attractive impurity of U=-5|t| while changing Eext
EF
(1010) SWNT with NO Eext while changing the strength of the attractive potential U
Changing Eext is different from changing U
SAMSUNG SDI FED ndash 2005 -
Picture1
Picture
2
Picture3
Picture
4
Power consumption of SED LCD PDP (36in)
SED
LCD
PDP
Canon-Toshiba SED at CEATEC2004
- Slide 1
- Slide 2
- Slide 3
- Slide 4
- Slide 5
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-
![Page 18: Jisoon Ihm School of Physics, Seoul National University](https://reader036.vdocuments.net/reader036/viewer/2022062723/56813b4d550346895da43eb8/html5/thumbnails/18.jpg)
Summary
bull Conductance of metallic CNTs with impurities and applied electric fields is studied
bull With N and B impurity atoms on opposite sides asymmetric switching is possible using external fields
bull With a large vacancy complex symmetric switching is possible using external fields
II Conformational Transform of Azobenzene Molecules
( B-Y Choi et al Phys Rev Lett 96 156106(2006) )
Azobenzene (AB) C6H5-N=N-C6H5
Transformation between transAB and cisAB
(Voltage bias using STM)
Geometries of tAB
Geometries of cAB
Optimal geometry of tAB and cAB
STS for tAB and cAB
Disperse Orange 3 (NH2-C6H4-N=N-C6H4-NO2)
Flat geometry of cAB
Summary
bull Electrical pulse is found to induce molecular flip between trans and cis structures
Example of MATERIAL DESIGN totalreflection by three nitrogen impurities
Doubly degenerate impurity states cause perfect reflection at 06 eV
(Both even and odd states are fully reflected at same energy)
Importance of geometric symmetry (equilateral triangle)
Appendix
Difference between Eext and impurity potential U
Lippman-Schwinger formalism
Eigenstate |ψgt of Htot associated with the eigenstate |gt of H0 with the same energy E (with impurity potential U at site )
Projection on to the impurity |gt
where
Reflection for the specific state |gt
Total transmission
Resonance condition
With applied electric fields
Suppose ∆H at site α is ∆E
In other words is G0(αE) shifted by ∆E
G0 projected at site
Effect of Eext Greenrsquos function itself changes
(1010) SWNT with single attractive impurity of U=-5|t|
(1010) SWNT with a single attractive impurity of U=-5|t| while changing Eext
EF
(1010) SWNT with NO Eext while changing the strength of the attractive potential U
Changing Eext is different from changing U
SAMSUNG SDI FED ndash 2005 -
Picture1
Picture
2
Picture3
Picture
4
Power consumption of SED LCD PDP (36in)
SED
LCD
PDP
Canon-Toshiba SED at CEATEC2004
- Slide 1
- Slide 2
- Slide 3
- Slide 4
- Slide 5
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![Page 19: Jisoon Ihm School of Physics, Seoul National University](https://reader036.vdocuments.net/reader036/viewer/2022062723/56813b4d550346895da43eb8/html5/thumbnails/19.jpg)
II Conformational Transform of Azobenzene Molecules
( B-Y Choi et al Phys Rev Lett 96 156106(2006) )
Azobenzene (AB) C6H5-N=N-C6H5
Transformation between transAB and cisAB
(Voltage bias using STM)
Geometries of tAB
Geometries of cAB
Optimal geometry of tAB and cAB
STS for tAB and cAB
Disperse Orange 3 (NH2-C6H4-N=N-C6H4-NO2)
Flat geometry of cAB
Summary
bull Electrical pulse is found to induce molecular flip between trans and cis structures
Example of MATERIAL DESIGN totalreflection by three nitrogen impurities
Doubly degenerate impurity states cause perfect reflection at 06 eV
(Both even and odd states are fully reflected at same energy)
Importance of geometric symmetry (equilateral triangle)
Appendix
Difference between Eext and impurity potential U
Lippman-Schwinger formalism
Eigenstate |ψgt of Htot associated with the eigenstate |gt of H0 with the same energy E (with impurity potential U at site )
Projection on to the impurity |gt
where
Reflection for the specific state |gt
Total transmission
Resonance condition
With applied electric fields
Suppose ∆H at site α is ∆E
In other words is G0(αE) shifted by ∆E
G0 projected at site
Effect of Eext Greenrsquos function itself changes
(1010) SWNT with single attractive impurity of U=-5|t|
(1010) SWNT with a single attractive impurity of U=-5|t| while changing Eext
EF
(1010) SWNT with NO Eext while changing the strength of the attractive potential U
Changing Eext is different from changing U
SAMSUNG SDI FED ndash 2005 -
Picture1
Picture
2
Picture3
Picture
4
Power consumption of SED LCD PDP (36in)
SED
LCD
PDP
Canon-Toshiba SED at CEATEC2004
- Slide 1
- Slide 2
- Slide 3
- Slide 4
- Slide 5
- Slide 6
- Slide 7
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-
![Page 20: Jisoon Ihm School of Physics, Seoul National University](https://reader036.vdocuments.net/reader036/viewer/2022062723/56813b4d550346895da43eb8/html5/thumbnails/20.jpg)
Azobenzene (AB) C6H5-N=N-C6H5
Transformation between transAB and cisAB
(Voltage bias using STM)
Geometries of tAB
Geometries of cAB
Optimal geometry of tAB and cAB
STS for tAB and cAB
Disperse Orange 3 (NH2-C6H4-N=N-C6H4-NO2)
Flat geometry of cAB
Summary
bull Electrical pulse is found to induce molecular flip between trans and cis structures
Example of MATERIAL DESIGN totalreflection by three nitrogen impurities
Doubly degenerate impurity states cause perfect reflection at 06 eV
(Both even and odd states are fully reflected at same energy)
Importance of geometric symmetry (equilateral triangle)
Appendix
Difference between Eext and impurity potential U
Lippman-Schwinger formalism
Eigenstate |ψgt of Htot associated with the eigenstate |gt of H0 with the same energy E (with impurity potential U at site )
Projection on to the impurity |gt
where
Reflection for the specific state |gt
Total transmission
Resonance condition
With applied electric fields
Suppose ∆H at site α is ∆E
In other words is G0(αE) shifted by ∆E
G0 projected at site
Effect of Eext Greenrsquos function itself changes
(1010) SWNT with single attractive impurity of U=-5|t|
(1010) SWNT with a single attractive impurity of U=-5|t| while changing Eext
EF
(1010) SWNT with NO Eext while changing the strength of the attractive potential U
Changing Eext is different from changing U
SAMSUNG SDI FED ndash 2005 -
Picture1
Picture
2
Picture3
Picture
4
Power consumption of SED LCD PDP (36in)
SED
LCD
PDP
Canon-Toshiba SED at CEATEC2004
- Slide 1
- Slide 2
- Slide 3
- Slide 4
- Slide 5
- Slide 6
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![Page 21: Jisoon Ihm School of Physics, Seoul National University](https://reader036.vdocuments.net/reader036/viewer/2022062723/56813b4d550346895da43eb8/html5/thumbnails/21.jpg)
Transformation between transAB and cisAB
(Voltage bias using STM)
Geometries of tAB
Geometries of cAB
Optimal geometry of tAB and cAB
STS for tAB and cAB
Disperse Orange 3 (NH2-C6H4-N=N-C6H4-NO2)
Flat geometry of cAB
Summary
bull Electrical pulse is found to induce molecular flip between trans and cis structures
Example of MATERIAL DESIGN totalreflection by three nitrogen impurities
Doubly degenerate impurity states cause perfect reflection at 06 eV
(Both even and odd states are fully reflected at same energy)
Importance of geometric symmetry (equilateral triangle)
Appendix
Difference between Eext and impurity potential U
Lippman-Schwinger formalism
Eigenstate |ψgt of Htot associated with the eigenstate |gt of H0 with the same energy E (with impurity potential U at site )
Projection on to the impurity |gt
where
Reflection for the specific state |gt
Total transmission
Resonance condition
With applied electric fields
Suppose ∆H at site α is ∆E
In other words is G0(αE) shifted by ∆E
G0 projected at site
Effect of Eext Greenrsquos function itself changes
(1010) SWNT with single attractive impurity of U=-5|t|
(1010) SWNT with a single attractive impurity of U=-5|t| while changing Eext
EF
(1010) SWNT with NO Eext while changing the strength of the attractive potential U
Changing Eext is different from changing U
SAMSUNG SDI FED ndash 2005 -
Picture1
Picture
2
Picture3
Picture
4
Power consumption of SED LCD PDP (36in)
SED
LCD
PDP
Canon-Toshiba SED at CEATEC2004
- Slide 1
- Slide 2
- Slide 3
- Slide 4
- Slide 5
- Slide 6
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-
![Page 22: Jisoon Ihm School of Physics, Seoul National University](https://reader036.vdocuments.net/reader036/viewer/2022062723/56813b4d550346895da43eb8/html5/thumbnails/22.jpg)
Geometries of tAB
Geometries of cAB
Optimal geometry of tAB and cAB
STS for tAB and cAB
Disperse Orange 3 (NH2-C6H4-N=N-C6H4-NO2)
Flat geometry of cAB
Summary
bull Electrical pulse is found to induce molecular flip between trans and cis structures
Example of MATERIAL DESIGN totalreflection by three nitrogen impurities
Doubly degenerate impurity states cause perfect reflection at 06 eV
(Both even and odd states are fully reflected at same energy)
Importance of geometric symmetry (equilateral triangle)
Appendix
Difference between Eext and impurity potential U
Lippman-Schwinger formalism
Eigenstate |ψgt of Htot associated with the eigenstate |gt of H0 with the same energy E (with impurity potential U at site )
Projection on to the impurity |gt
where
Reflection for the specific state |gt
Total transmission
Resonance condition
With applied electric fields
Suppose ∆H at site α is ∆E
In other words is G0(αE) shifted by ∆E
G0 projected at site
Effect of Eext Greenrsquos function itself changes
(1010) SWNT with single attractive impurity of U=-5|t|
(1010) SWNT with a single attractive impurity of U=-5|t| while changing Eext
EF
(1010) SWNT with NO Eext while changing the strength of the attractive potential U
Changing Eext is different from changing U
SAMSUNG SDI FED ndash 2005 -
Picture1
Picture
2
Picture3
Picture
4
Power consumption of SED LCD PDP (36in)
SED
LCD
PDP
Canon-Toshiba SED at CEATEC2004
- Slide 1
- Slide 2
- Slide 3
- Slide 4
- Slide 5
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-
![Page 23: Jisoon Ihm School of Physics, Seoul National University](https://reader036.vdocuments.net/reader036/viewer/2022062723/56813b4d550346895da43eb8/html5/thumbnails/23.jpg)
Geometries of cAB
Optimal geometry of tAB and cAB
STS for tAB and cAB
Disperse Orange 3 (NH2-C6H4-N=N-C6H4-NO2)
Flat geometry of cAB
Summary
bull Electrical pulse is found to induce molecular flip between trans and cis structures
Example of MATERIAL DESIGN totalreflection by three nitrogen impurities
Doubly degenerate impurity states cause perfect reflection at 06 eV
(Both even and odd states are fully reflected at same energy)
Importance of geometric symmetry (equilateral triangle)
Appendix
Difference between Eext and impurity potential U
Lippman-Schwinger formalism
Eigenstate |ψgt of Htot associated with the eigenstate |gt of H0 with the same energy E (with impurity potential U at site )
Projection on to the impurity |gt
where
Reflection for the specific state |gt
Total transmission
Resonance condition
With applied electric fields
Suppose ∆H at site α is ∆E
In other words is G0(αE) shifted by ∆E
G0 projected at site
Effect of Eext Greenrsquos function itself changes
(1010) SWNT with single attractive impurity of U=-5|t|
(1010) SWNT with a single attractive impurity of U=-5|t| while changing Eext
EF
(1010) SWNT with NO Eext while changing the strength of the attractive potential U
Changing Eext is different from changing U
SAMSUNG SDI FED ndash 2005 -
Picture1
Picture
2
Picture3
Picture
4
Power consumption of SED LCD PDP (36in)
SED
LCD
PDP
Canon-Toshiba SED at CEATEC2004
- Slide 1
- Slide 2
- Slide 3
- Slide 4
- Slide 5
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-
![Page 24: Jisoon Ihm School of Physics, Seoul National University](https://reader036.vdocuments.net/reader036/viewer/2022062723/56813b4d550346895da43eb8/html5/thumbnails/24.jpg)
Optimal geometry of tAB and cAB
STS for tAB and cAB
Disperse Orange 3 (NH2-C6H4-N=N-C6H4-NO2)
Flat geometry of cAB
Summary
bull Electrical pulse is found to induce molecular flip between trans and cis structures
Example of MATERIAL DESIGN totalreflection by three nitrogen impurities
Doubly degenerate impurity states cause perfect reflection at 06 eV
(Both even and odd states are fully reflected at same energy)
Importance of geometric symmetry (equilateral triangle)
Appendix
Difference between Eext and impurity potential U
Lippman-Schwinger formalism
Eigenstate |ψgt of Htot associated with the eigenstate |gt of H0 with the same energy E (with impurity potential U at site )
Projection on to the impurity |gt
where
Reflection for the specific state |gt
Total transmission
Resonance condition
With applied electric fields
Suppose ∆H at site α is ∆E
In other words is G0(αE) shifted by ∆E
G0 projected at site
Effect of Eext Greenrsquos function itself changes
(1010) SWNT with single attractive impurity of U=-5|t|
(1010) SWNT with a single attractive impurity of U=-5|t| while changing Eext
EF
(1010) SWNT with NO Eext while changing the strength of the attractive potential U
Changing Eext is different from changing U
SAMSUNG SDI FED ndash 2005 -
Picture1
Picture
2
Picture3
Picture
4
Power consumption of SED LCD PDP (36in)
SED
LCD
PDP
Canon-Toshiba SED at CEATEC2004
- Slide 1
- Slide 2
- Slide 3
- Slide 4
- Slide 5
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-
![Page 25: Jisoon Ihm School of Physics, Seoul National University](https://reader036.vdocuments.net/reader036/viewer/2022062723/56813b4d550346895da43eb8/html5/thumbnails/25.jpg)
STS for tAB and cAB
Disperse Orange 3 (NH2-C6H4-N=N-C6H4-NO2)
Flat geometry of cAB
Summary
bull Electrical pulse is found to induce molecular flip between trans and cis structures
Example of MATERIAL DESIGN totalreflection by three nitrogen impurities
Doubly degenerate impurity states cause perfect reflection at 06 eV
(Both even and odd states are fully reflected at same energy)
Importance of geometric symmetry (equilateral triangle)
Appendix
Difference between Eext and impurity potential U
Lippman-Schwinger formalism
Eigenstate |ψgt of Htot associated with the eigenstate |gt of H0 with the same energy E (with impurity potential U at site )
Projection on to the impurity |gt
where
Reflection for the specific state |gt
Total transmission
Resonance condition
With applied electric fields
Suppose ∆H at site α is ∆E
In other words is G0(αE) shifted by ∆E
G0 projected at site
Effect of Eext Greenrsquos function itself changes
(1010) SWNT with single attractive impurity of U=-5|t|
(1010) SWNT with a single attractive impurity of U=-5|t| while changing Eext
EF
(1010) SWNT with NO Eext while changing the strength of the attractive potential U
Changing Eext is different from changing U
SAMSUNG SDI FED ndash 2005 -
Picture1
Picture
2
Picture3
Picture
4
Power consumption of SED LCD PDP (36in)
SED
LCD
PDP
Canon-Toshiba SED at CEATEC2004
- Slide 1
- Slide 2
- Slide 3
- Slide 4
- Slide 5
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-
![Page 26: Jisoon Ihm School of Physics, Seoul National University](https://reader036.vdocuments.net/reader036/viewer/2022062723/56813b4d550346895da43eb8/html5/thumbnails/26.jpg)
Disperse Orange 3 (NH2-C6H4-N=N-C6H4-NO2)
Flat geometry of cAB
Summary
bull Electrical pulse is found to induce molecular flip between trans and cis structures
Example of MATERIAL DESIGN totalreflection by three nitrogen impurities
Doubly degenerate impurity states cause perfect reflection at 06 eV
(Both even and odd states are fully reflected at same energy)
Importance of geometric symmetry (equilateral triangle)
Appendix
Difference between Eext and impurity potential U
Lippman-Schwinger formalism
Eigenstate |ψgt of Htot associated with the eigenstate |gt of H0 with the same energy E (with impurity potential U at site )
Projection on to the impurity |gt
where
Reflection for the specific state |gt
Total transmission
Resonance condition
With applied electric fields
Suppose ∆H at site α is ∆E
In other words is G0(αE) shifted by ∆E
G0 projected at site
Effect of Eext Greenrsquos function itself changes
(1010) SWNT with single attractive impurity of U=-5|t|
(1010) SWNT with a single attractive impurity of U=-5|t| while changing Eext
EF
(1010) SWNT with NO Eext while changing the strength of the attractive potential U
Changing Eext is different from changing U
SAMSUNG SDI FED ndash 2005 -
Picture1
Picture
2
Picture3
Picture
4
Power consumption of SED LCD PDP (36in)
SED
LCD
PDP
Canon-Toshiba SED at CEATEC2004
- Slide 1
- Slide 2
- Slide 3
- Slide 4
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-
![Page 27: Jisoon Ihm School of Physics, Seoul National University](https://reader036.vdocuments.net/reader036/viewer/2022062723/56813b4d550346895da43eb8/html5/thumbnails/27.jpg)
Flat geometry of cAB
Summary
bull Electrical pulse is found to induce molecular flip between trans and cis structures
Example of MATERIAL DESIGN totalreflection by three nitrogen impurities
Doubly degenerate impurity states cause perfect reflection at 06 eV
(Both even and odd states are fully reflected at same energy)
Importance of geometric symmetry (equilateral triangle)
Appendix
Difference between Eext and impurity potential U
Lippman-Schwinger formalism
Eigenstate |ψgt of Htot associated with the eigenstate |gt of H0 with the same energy E (with impurity potential U at site )
Projection on to the impurity |gt
where
Reflection for the specific state |gt
Total transmission
Resonance condition
With applied electric fields
Suppose ∆H at site α is ∆E
In other words is G0(αE) shifted by ∆E
G0 projected at site
Effect of Eext Greenrsquos function itself changes
(1010) SWNT with single attractive impurity of U=-5|t|
(1010) SWNT with a single attractive impurity of U=-5|t| while changing Eext
EF
(1010) SWNT with NO Eext while changing the strength of the attractive potential U
Changing Eext is different from changing U
SAMSUNG SDI FED ndash 2005 -
Picture1
Picture
2
Picture3
Picture
4
Power consumption of SED LCD PDP (36in)
SED
LCD
PDP
Canon-Toshiba SED at CEATEC2004
- Slide 1
- Slide 2
- Slide 3
- Slide 4
- Slide 5
- Slide 6
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-
![Page 28: Jisoon Ihm School of Physics, Seoul National University](https://reader036.vdocuments.net/reader036/viewer/2022062723/56813b4d550346895da43eb8/html5/thumbnails/28.jpg)
Summary
bull Electrical pulse is found to induce molecular flip between trans and cis structures
Example of MATERIAL DESIGN totalreflection by three nitrogen impurities
Doubly degenerate impurity states cause perfect reflection at 06 eV
(Both even and odd states are fully reflected at same energy)
Importance of geometric symmetry (equilateral triangle)
Appendix
Difference between Eext and impurity potential U
Lippman-Schwinger formalism
Eigenstate |ψgt of Htot associated with the eigenstate |gt of H0 with the same energy E (with impurity potential U at site )
Projection on to the impurity |gt
where
Reflection for the specific state |gt
Total transmission
Resonance condition
With applied electric fields
Suppose ∆H at site α is ∆E
In other words is G0(αE) shifted by ∆E
G0 projected at site
Effect of Eext Greenrsquos function itself changes
(1010) SWNT with single attractive impurity of U=-5|t|
(1010) SWNT with a single attractive impurity of U=-5|t| while changing Eext
EF
(1010) SWNT with NO Eext while changing the strength of the attractive potential U
Changing Eext is different from changing U
SAMSUNG SDI FED ndash 2005 -
Picture1
Picture
2
Picture3
Picture
4
Power consumption of SED LCD PDP (36in)
SED
LCD
PDP
Canon-Toshiba SED at CEATEC2004
- Slide 1
- Slide 2
- Slide 3
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Example of MATERIAL DESIGN totalreflection by three nitrogen impurities
Doubly degenerate impurity states cause perfect reflection at 06 eV
(Both even and odd states are fully reflected at same energy)
Importance of geometric symmetry (equilateral triangle)
Appendix
Difference between Eext and impurity potential U
Lippman-Schwinger formalism
Eigenstate |ψgt of Htot associated with the eigenstate |gt of H0 with the same energy E (with impurity potential U at site )
Projection on to the impurity |gt
where
Reflection for the specific state |gt
Total transmission
Resonance condition
With applied electric fields
Suppose ∆H at site α is ∆E
In other words is G0(αE) shifted by ∆E
G0 projected at site
Effect of Eext Greenrsquos function itself changes
(1010) SWNT with single attractive impurity of U=-5|t|
(1010) SWNT with a single attractive impurity of U=-5|t| while changing Eext
EF
(1010) SWNT with NO Eext while changing the strength of the attractive potential U
Changing Eext is different from changing U
SAMSUNG SDI FED ndash 2005 -
Picture1
Picture
2
Picture3
Picture
4
Power consumption of SED LCD PDP (36in)
SED
LCD
PDP
Canon-Toshiba SED at CEATEC2004
- Slide 1
- Slide 2
- Slide 3
- Slide 4
- Slide 5
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Difference between Eext and impurity potential U
Lippman-Schwinger formalism
Eigenstate |ψgt of Htot associated with the eigenstate |gt of H0 with the same energy E (with impurity potential U at site )
Projection on to the impurity |gt
where
Reflection for the specific state |gt
Total transmission
Resonance condition
With applied electric fields
Suppose ∆H at site α is ∆E
In other words is G0(αE) shifted by ∆E
G0 projected at site
Effect of Eext Greenrsquos function itself changes
(1010) SWNT with single attractive impurity of U=-5|t|
(1010) SWNT with a single attractive impurity of U=-5|t| while changing Eext
EF
(1010) SWNT with NO Eext while changing the strength of the attractive potential U
Changing Eext is different from changing U
SAMSUNG SDI FED ndash 2005 -
Picture1
Picture
2
Picture3
Picture
4
Power consumption of SED LCD PDP (36in)
SED
LCD
PDP
Canon-Toshiba SED at CEATEC2004
- Slide 1
- Slide 2
- Slide 3
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Projection on to the impurity |gt
where
Reflection for the specific state |gt
Total transmission
Resonance condition
With applied electric fields
Suppose ∆H at site α is ∆E
In other words is G0(αE) shifted by ∆E
G0 projected at site
Effect of Eext Greenrsquos function itself changes
(1010) SWNT with single attractive impurity of U=-5|t|
(1010) SWNT with a single attractive impurity of U=-5|t| while changing Eext
EF
(1010) SWNT with NO Eext while changing the strength of the attractive potential U
Changing Eext is different from changing U
SAMSUNG SDI FED ndash 2005 -
Picture1
Picture
2
Picture3
Picture
4
Power consumption of SED LCD PDP (36in)
SED
LCD
PDP
Canon-Toshiba SED at CEATEC2004
- Slide 1
- Slide 2
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With applied electric fields
Suppose ∆H at site α is ∆E
In other words is G0(αE) shifted by ∆E
G0 projected at site
Effect of Eext Greenrsquos function itself changes
(1010) SWNT with single attractive impurity of U=-5|t|
(1010) SWNT with a single attractive impurity of U=-5|t| while changing Eext
EF
(1010) SWNT with NO Eext while changing the strength of the attractive potential U
Changing Eext is different from changing U
SAMSUNG SDI FED ndash 2005 -
Picture1
Picture
2
Picture3
Picture
4
Power consumption of SED LCD PDP (36in)
SED
LCD
PDP
Canon-Toshiba SED at CEATEC2004
- Slide 1
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(1010) SWNT with single attractive impurity of U=-5|t|
(1010) SWNT with a single attractive impurity of U=-5|t| while changing Eext
EF
(1010) SWNT with NO Eext while changing the strength of the attractive potential U
Changing Eext is different from changing U
SAMSUNG SDI FED ndash 2005 -
Picture1
Picture
2
Picture3
Picture
4
Power consumption of SED LCD PDP (36in)
SED
LCD
PDP
Canon-Toshiba SED at CEATEC2004
- Slide 1
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(1010) SWNT with a single attractive impurity of U=-5|t| while changing Eext
EF
(1010) SWNT with NO Eext while changing the strength of the attractive potential U
Changing Eext is different from changing U
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Power consumption of SED LCD PDP (36in)
SED
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PDP
Canon-Toshiba SED at CEATEC2004
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SAMSUNG SDI FED ndash 2005 -
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Power consumption of SED LCD PDP (36in)
SED
LCD
PDP
Canon-Toshiba SED at CEATEC2004
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Power consumption of SED LCD PDP (36in)
SED
LCD
PDP
Canon-Toshiba SED at CEATEC2004
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