SLIDE 1
r stt t sr - - PowerPoint PPT Presentation
r stt t sr - - PowerPoint PPT Presentation
r stt t sr srr t str P s P strs
SLIDE 2
SLIDE 3
❙✉r❢❛❝❡ st❛t❡s ♦❢ ❛ ✸❉ ❚■ ✇✐t❤ T ✲s②♠♠❡tr②
◮ ❙✐♥❣❧❡ ❉✐r❛❝ ❝♦♥❡ ✭❇✐✷❙❡✸, ❇✐✷❚❡✸ ❡t❝✮
❍✵ = ✈❢ (s · ♣),
◮ ❙♣✐♥✲♣♦❧❛r✐③❡❞ ❡❧❡❝tr♦♥ st❛t❡s
Ψ =
- ✶
± ♣①+✐♣②
|♣|
- ❡✐♣·r
❊ = ±✈❢ |♣|
◮ T ✲s②♠♠❡tr② ❝♦♥♥❡❝ts st❛t❡s ✇✐t❤ ♦♣♣♦s✐t❡ ♣ ❛♥❞ s✳
SLIDE 4
▼❛❥♦r❛♥❛ ❢❡r♠✐♦♥ ✐♥ ❛ ✈♦rt❡① ❝♦r❡
m m
usual s-wave SC
spinless p-wave SC or s-wave on top
- f TI surface
◮ s✲✇❛✈❡ s✉♣❡r❝♦♥❞✉❝t✐✈✐t② ✐s ✐♥❞✉❝❡❞ ❜② ♣r♦①✐♠✐t② ❡✛❡❝t ◮ ✈♦rt❡① ❜r❡❛❦s T ✲s②♠♠❡tr② ❛♥❞ ♣r♦❞✉❝❡s ❛♥ ♦❞❞ ❤❛♠✐❧t♦♥✐❛♥✿
❍ = (✈❢ s · ♣ − µ)τ③ + ∆(r)(τ① ❝♦s θ + τ② s✐♥ θ)
◮ ♥♦♥✲❞❡❣❡♥❡r❛t❡ ❞❡ ●❡♥♥❡s s♣❡❝tr✉♠
❊♠ = ω✵♠, ω✵ ∼ ∆✷/❊❢ ,
◮ ♠ = ✵ ✐s ❛ ▼❛❥♦r❛♥❛ st❛t❡ ✭❋✉✱ ❑❛♥❡✱ ✷✵✵✽✮
SLIDE 5
❙❡t✉♣ ❛♥❞ ●♦❛❧
Topological Insulator SC
h 2e
Tunneling probe
Strong disorder changes subgap spectrum significantly Majorana level is protected by symmetry and stays at E=0
✇❡ ✜♥❞
◮ ❛✈❡r❛❣❡ ❧♦❝❛❧ ❞❡♥s✐t② ♦❢ st❛t❡s ✭❉♦❙✮ ρ(r, ❊)✱ ◮ ■(❱ , ❚) ❝❤❛r❛❝t❡r✐st✐❝s ♦❢ ❛ t✉♥♥❡❧✐♥❣ ♣r♦❜❡ ❛♣♣❧✐❡❞ t♦ t❤❡ ❚■
s✉r❢❛❝❡ ❢♦r ❛♥② ♣❛rt✐❝✉❧❛r ❞✐s♦r❞❡r r❡❛❧✐③❛t✐♦♥ ❛♥❞ t❤❡ ❛✈❡r❛❣❡✳
◮ s♣❡❝✐❛❧ ❜❡❤❛✈✐♦✉r ❛t ③❡r♦✲❜✐❛s✿ ✷❡✷/❤ ♣❡❛❦ ❢♦r ❇✲❝❧❛ss
✭❡♥s❡♠❜❧❡ ✇✐t❤ ▼❛❥♦r❛♥❛ ❢❡r♠✐♦♥✮ ❛♥❞ ❞✐♣ t♦ ③❡r♦ ❢♦r ❉✲❝❧❛ss ✭♥♦ ▼❛❥♦r❛♥❛ ❢❡r♠✐♦♥✮
SLIDE 6
❍❛♠✐❧t♦♥✐❛♥
◮ ❚❤❡ ❞✐s♦r❞❡r❡❞ s✉♣❡r❝♦♥❞✉❝t✐♥❣ ❚■ s✉r❢❛❝❡ ✐s ❞❡s❝r✐❜❡❞ ❜②
❍ = (✈❢ s · ♣ − µ + ❱ (r))τ③ + ∆(r)(τ① ❝♦s θ + τ② s✐♥ θ) ✇✐t❤ ✇❤✐t❡✲♥♦✐s❡ ❞✐s♦r❞❡r ♣♦t❡♥t✐❛❧ ❱ (r)✿ ❱ (r)❱ (r′) = δ(r − r′) πντ ❲❡ ❝♦♥s✐❞❡r t❤❡ r❡❣✐♠❡ ❊❚❤ = ❉/❘✷ ≪ ∆ ≪ ❊❢ ✱ ✐♠♣❧②✐♥❣ ∆(r) =
- ✵,
r < ❘, ∆, r ≥ ❘.
SLIDE 7
❍❛♠✐❧t♦♥✐❛♥
◮ ❚❤❡ ❞✐s♦r❞❡r❡❞ s✉♣❡r❝♦♥❞✉❝t✐♥❣ ❚■ s✉r❢❛❝❡ ✐s ❞❡s❝r✐❜❡❞ ❜②
❍ = (✈❢ s · ♣ − µ + ❱ (r))τ③ + ∆(r)(τ① ❝♦s θ + τ② s✐♥ θ) ✇✐t❤ ✇❤✐t❡✲♥♦✐s❡ ❞✐s♦r❞❡r ♣♦t❡♥t✐❛❧ ❱ (r)✿ ❱ (r)❱ (r′) = δ(r − r′) πντ
◮ ❲❡ ❝♦♥s✐❞❡r t❤❡ r❡❣✐♠❡ ❊❚❤ = ❉/❘✷ ≪ ∆ ≪ ❊❢ ✱ ✐♠♣❧②✐♥❣
∆(r) =
- ✵,
r < ❘, ∆, r ≥ ❘.
SLIDE 8
❙✉♣❡rs②♠♠❡tr✐❝ s✐❣♠❛✲♠♦❞❡❧ ❛❝t✐♦♥
❙[◗] = πν ✽
- ❞✷ rstr [❉(∇◗)✷ + ✹(✐ǫΛ − ˆ
∆)◗]+❙θ[◗]
◮ ◗ ✐s ❛ ✽ × ✽ s✉♣❡r♠❛tr✐① ✐♥ ◆❛♠❜✉✲●♦r✬❦♦✈ ✭τ✮ ❛♥❞
P❛rt✐❝❧❡✲❍♦❧❡ ✭σ✮ s♣❛❝❡✱ ♦❜❡②✐♥❣ ◗✷ = ✶ ❛♥❞ ◗ = ❈◗❚❈ ❚ ✇✐t❤ ❈ = τ① σ① ✵ ✵ ✐σ②
- ❋❇
, t❤❡ ❉✐r❛❝ s♣❡❝tr✉♠ ♣r♦❞✉❝❡s ❛ t♦♣♦❧♦❣✐❝❛❧ t❡r♠ ❙θ[◗]✱ ǫ = ❊ + ✐●tδ(r − r✵)/✹πν ✇✐t❤ ❊ ❜❡✐♥❣ t❤❡ ❡♥❡r❣② ❛♥❞ t❤❡ s❡❝♦♥❞ t❡r♠ ❞❡s❝r✐❜✐♥❣ t✉♥♥❡❧✐♥❣ t♦ t❤❡ ♣r♦❜❡❀ Λ = σ③τ③✳ ♣❧❛❝❡❤♦❧❞❡r
SLIDE 9
❙✉♣❡rs②♠♠❡tr✐❝ s✐❣♠❛✲♠♦❞❡❧ ❛❝t✐♦♥
❙[◗] = πν ✽
- ❞✷ rstr [❉(∇◗)✷ + ✹(✐ǫΛ − ˆ
∆)◗]+❙θ[◗]
◮ ◗ ✐s ❛ ✽ × ✽ s✉♣❡r♠❛tr✐① ✐♥ ◆❛♠❜✉✲●♦r✬❦♦✈ ✭τ✮ ❛♥❞
P❛rt✐❝❧❡✲❍♦❧❡ ✭σ✮ s♣❛❝❡✱ ♦❜❡②✐♥❣ ◗✷ = ✶ ❛♥❞ ◗ = ❈◗❚❈ ❚ ✇✐t❤ ❈ = τ① σ① ✵ ✵ ✐σ②
- ❋❇
,
◮ t❤❡ ❉✐r❛❝ s♣❡❝tr✉♠ ♣r♦❞✉❝❡s ❛ t♦♣♦❧♦❣✐❝❛❧ t❡r♠ ❙θ[◗]✱
ǫ = ❊ + ✐●tδ(r − r✵)/✹πν ✇✐t❤ ❊ ❜❡✐♥❣ t❤❡ ❡♥❡r❣② ❛♥❞ t❤❡ s❡❝♦♥❞ t❡r♠ ❞❡s❝r✐❜✐♥❣ t✉♥♥❡❧✐♥❣ t♦ t❤❡ ♣r♦❜❡❀ Λ = σ③τ③✳ ♣❧❛❝❡❤♦❧❞❡r
SLIDE 10
❙✉♣❡rs②♠♠❡tr✐❝ s✐❣♠❛✲♠♦❞❡❧ ❛❝t✐♦♥
❙[◗] = πν ✽
- ❞✷ rstr [❉(∇◗)✷ + ✹(✐ǫΛ − ˆ
∆)◗]+❙θ[◗]
◮ ◗ ✐s ❛ ✽ × ✽ s✉♣❡r♠❛tr✐① ✐♥ ◆❛♠❜✉✲●♦r✬❦♦✈ ✭τ✮ ❛♥❞
P❛rt✐❝❧❡✲❍♦❧❡ ✭σ✮ s♣❛❝❡✱ ♦❜❡②✐♥❣ ◗✷ = ✶ ❛♥❞ ◗ = ❈◗❚❈ ❚ ✇✐t❤ ❈ = τ① σ① ✵ ✵ ✐σ②
- ❋❇
,
◮ t❤❡ ❉✐r❛❝ s♣❡❝tr✉♠ ♣r♦❞✉❝❡s ❛ t♦♣♦❧♦❣✐❝❛❧ t❡r♠ ❙θ[◗]✱ ◮ ǫ = ❊ + ✐●tδ(r − r✵)/✹πν ✇✐t❤ ❊ ❜❡✐♥❣ t❤❡ ❡♥❡r❣② ❛♥❞ t❤❡
s❡❝♦♥❞ t❡r♠ ❞❡s❝r✐❜✐♥❣ t✉♥♥❡❧✐♥❣ t♦ t❤❡ ♣r♦❜❡❀ Λ = σ③τ③✳ ♣❧❛❝❡❤♦❧❞❡r
SLIDE 11
❙[◗] = πν ✽
- ❞✷ rstr [❉(∇◗)✷ + ✹(✐ǫΛ − ˆ
∆)◗] + ❙θ[◗] ❈♦♥❞✐t✐♦♥s ◗✷ = ✶ ❛♥❞ ◗ = ◗ ❧❡❛❞ t♦ t❤❡ str✉❝t✉r❡✿ ◗ = ❱ −✶ ◗❋ ✵ ✵ ◗❇
- ❱
✇❤❡r❡ ❱ ❝♦♥t❛✐♥s ✽ ❣r❛ss♠❛♥ ✈❛r✐❛❜❧❡s✱ ❛♥❞ ◗❋,❇ ❛r❡ ♣❛r❛♠❡t❡r✐③❡❞ ❜② ✹ ❛♥❣❧❡s ❡❛❝❤✳ ◗❋,❇ = ◗❋,❇✳
SLIDE 12
❙[◗] = πν ✽
- ❞✷ rstr [❉(∇◗)✷ + ✹(✐ǫΛ − ˆ
∆)◗] + ❙θ[◗]
x
SLIDE 13
❙[◗] = πν ✽
- ❞✷ rstr [❉(∇◗)✷ + ✹(✐ǫΛ − ˆ
∆)◗] + ❙θ[◗]
x
variation at zero energy: Usadel equation
vortex term at origin
SLIDE 14
❙[◗] = πν ✽
- ❞✷ rstr [❉(∇◗)✷ + ✹(✐ǫΛ − ˆ
∆)◗] + ❙θ[◗]
U
structure of the symmetry class D, Change in means D-odd
manifold consists of two disjoint parts
SLIDE 15
❉❡♥s✐t② ♦❢ st❛t❡s ❛t ❧♦✇ ❡♥❡r❣✐❡s
ρ(r, ❊) = ν ✽ ❘❡
- ❉◗ ❙tr[ˆ
❦Λ◗(r)] ❡−❙[◗]. ❚✇♦ ♠❛♥✐❢♦❧❞ ♣❛rts ❝♦♥tr✐❜✉t❡ t♦ t❤✐s ✐♥t❡❣r❛❧ ✇✐t❤ ♦♣♣♦s✐t❡ s✐❣♥s✱ ✇❤✐❝❤ ❞✐st✐♥❣✉✐s❤❡s t❤❡ ❉✲♦❞❞ ✭❇✮ ❝❧❛ss ❢r♦♠ ❉✲❡✈❡♥✳ ❲❡ ✜♥❞ ❢♦r ❊ ≪ ❊❚❤ ρ(r, ❊) = ν ♥(r)❢ (❊/ω✵), ♥(r) = ❝♦s θ✶(r) = ❘✷ − r✷ ❘✷ + r✷ , ❢ (①) = γ π(①✷ + γ✷) + ✶ − s✐♥(✷π①) ✷π① . ✇❤❡r❡ γ = ●t♥(r✵)/✷π ≪ ✶ ✇✐t❤ r✵ ❜❡✐♥❣ t❤❡ ♣♦s✐t✐♦♥ ♦❢ t❤❡ ♣r♦❜❡✱ ❛♥❞ t❤❡ ❧❡✈❡❧✲s♣❛❝✐♥❣ ω−✶
✵
= ✷ν
- ❞✷r ❝♦s θ✶(r) = ✷π(❧♦❣ ✹ − ✶)ν❘✷
SLIDE 16
❉❡♥s✐t② ♦❢ st❛t❡s ❛t ❧♦✇ ❡♥❡r❣✐❡s
ρ(r, ❊) = ν ✽ ❘❡
- ❉◗ ❙tr[ˆ
❦Λ◗(r)] ❡−❙[◗]. ❚✇♦ ♠❛♥✐❢♦❧❞ ♣❛rts ❝♦♥tr✐❜✉t❡ t♦ t❤✐s ✐♥t❡❣r❛❧ ✇✐t❤ ♦♣♣♦s✐t❡ s✐❣♥s✱ ✇❤✐❝❤ ❞✐st✐♥❣✉✐s❤❡s t❤❡ ❉✲♦❞❞ ✭❇✮ ❝❧❛ss ❢r♦♠ ❉✲❡✈❡♥✳ ❲❡ ✜♥❞ ❢♦r ❊ ≪ ❊❚❤ ρ(r, ❊) = ν ♥(r)❢ (❊/ω✵), ♥(r) = ❝♦s θ✶(r) = ❘✷ − r✷ ❘✷ + r✷ , ❢ (①) = γ π(①✷ + γ✷) + ✶ − s✐♥(✷π①) ✷π① . ✇❤❡r❡ γ = ●t♥(r✵)/✷π ≪ ✶ ✇✐t❤ r✵ ❜❡✐♥❣ t❤❡ ♣♦s✐t✐♦♥ ♦❢ t❤❡ ♣r♦❜❡✱ ❛♥❞ t❤❡ ❧❡✈❡❧✲s♣❛❝✐♥❣ ω−✶
✵
= ✷ν
- ❞✷r ❝♦s θ✶(r) = ✷π(❧♦❣ ✹ − ✶)ν❘✷
SLIDE 17
0.5 1.0 1.5 2.0 0.2 0.4 0.6 0.8 1.0
νD=10
E, ETh N(E), πνR
2
■♥t❡❣r❛t✐♥❣ ρ(r, ❊) ♦✈❡r ❞✷r ✇❡ ♦❜t❛✐♥ ◆(❊) = γ ✷π(❊ ✷/ω✵ + γ✷ω✵) + ✶ ✷ω✵
- ✶ − s✐♥(✷π❊/ω✵)
✷π❊/ω✵
- ❲❤❡♥ ●t = ✵ ✭♥♦ ♣r♦❜❡✮ t❤❡ ✜rst t❡r♠ ❜❡❝♦♠❡s δ(❊)/✷✱
❝❤❛r❛❝t❡r✐st✐❝ ❢♦r t❤❡ ❇✲❝❧❛ss ✭❉✳ ❆✳ ■✈❛♥♦✈✱ ✷✵✵✷✮✳
SLIDE 18
❚✉♥♥❡❧✐♥❣ ❝✉rr❡♥t
❚❤❡ ❝✉rr❡♥t ✐♥ ❛ t✉♥♥❡❧✐♥❣ ❡①♣❡r✐♠❡♥t ✐s ■ = ❡●t ❤ν
- ρ(❊, r✵)
- ❢ (❊ − ❡❱ ) − ❢ (❊)
- ❞❊
✇✐t❤ t❤❡ ❋❡r♠✐ ❞✐str✐❜✉t✐♦♥ ❢✉♥❝t✐♦♥ ❢ (❊)✳ ❆t ❡❱ ≪ ω✵ ✇❡ ❣❡t ❞■ ❞❱ = ✷❡✷γ✷ ❤
- γ✷ + (❡❱ /ω✵)✷,
❚ ≪ γω✵, π❡✷γω✵ ✷❤❚ ❝♦s❤✷(❡❱ /✷❚) , γω✵ ≪ ❚ ≪ ω✵. ❆t s♠❛❧❧ ❚ t❤❡r❡ ✐s ❛ ▲♦r❡♥t③ ♣❡❛❦ ❛t ❊ = ✵ ✇✐t❤ ❛ ✇✐❞t❤ ∼ ●tω✵ ❛♥❞ ❛ ✉♥✐✈❡rs❛❧ ❤❡✐❣❤t ❡✷/π ♠❡❛♥✐♥❣ ♣❡r❢❡❝t ❆♥❞r❡❡✈ r❡✢❡❝t✐♦♥ ✭▲❛✇✱ ▲❡❡✱ ◆❣✱ ✷✵✵✾✮✳
SLIDE 19
1 1 eV Ω0 dIdV e2Π Gt T0 TΓ 1
◮ ❆❧❧ ❧❡✈❡❧s ♣r♦❞✉❝❡ ▲♦r❡♥t③✲s❤❛♣❡❞ r❡s♦♥❛♥❝❡s❀ ◮ ❍❡✐❣❤ts ❡q✉❛❧ ✷❡✷ ❤ ψ†Cψ ψ†ψ ✱ ✇✐❞t❤s ❡q✉❛❧ ●t ψ†ψ ν ❀ ◮ ❋❡r♠✐♦♥✐❝ ❧❡✈❡❧s ♣r♦❞✉❝❡ t✇♦ ♣❡❛❦s ❛t ±❊✱ ▼❛❥♦r❛♥❛ ❧❡✈❡❧
❝r❡❛t❡s ♦♥❡ ♣❡❛❦ ❛t ❊ = ✵✳ ❋♦r ❉✲❡✈❡♥ ■(✵) ≡ ✵✳
SLIDE 20
③❡r♦✲❜✐❛s ❝♦♥❞✉❝t❛♥❝❡ ❞✐♣ ✐♥ ❝❧❛ss ❉
Symmetric levels interfere destructively, at E=0 Andreev reflection is absent Andreev reflection probability At small voltages Andreev current is suppressed, dI/dV is not proportional to DoS any more DoS dI/dV E eV
◮ ❊①❛❝t❧② ❛t ❊ = ✵ ❝♦♥❞✉❝t❛♥❝❡ ✐s ❡✐t❤❡r ✵ ♦r ✷❡✷/✳ ❚❤✐s
❢♦❧❧♦✇s ❢r♦♠ ❇❞●✲s②♠♠❡tr② ❛♥❞ ✉♥✐t❛r✐t② ❢♦r ❛ s✐♥❣❧❡✲❝❤❛♥♥❡❧ ❙✲♠❛tr✐①✳
◮ ✐♥ ❉✲❝❧❛ss ✭♥♦ ▼❛❥♦r❛♥❛ ❢❡r♠✐♦♥✮ ❞■/❞❱ = ✵✳ Pr♦❝❡ss❡s
✐♥✈♦❧✈✐♥❣ s②♠♠❡tr✐❝ ❆♥❞r❡❡✈ ❧❡✈❡❧s ±❊❥ ❝❛♥❝❡❧ ❡❛❝❤ ♦t❤❡r ♦✉t
◮ ✐♥ ❇✲❝❧❛ss ✭♦♥❡ ▼❛❥♦r❛♥❛ ❢❡r♠✐♦♥✮ ❞■/❞❱ = ✷❡✷/ ✇❤✐❝❤ ✐s
t❤❡ ▼❛❥♦r❛♥❛ ❢❡r♠✐♦♥ ❝♦♥tr✐❜✉t✐♦♥
SLIDE 21
❈♦♥❝❧✉s✐♦♥s
❈♦♥❝❧✉s✐♦♥s ❬P❘❇✱ ✽✻✱ ✵✸✺✹✹✶ ✭✷✵✶✷✮❪
◮ ❚✉♥♥❡❧✐♥❣ ❝✉rr❡♥t ✐♥ ❛ ✈♦rt❡① ❝♦r❡ ♦♥ ❛ ❚■ s✉r❢❛❝❡ ❤❛s ❜❡❡♥
st✉❞✐❡❞ ✐♥ t❤❡ str♦♥❣ ❞✐s♦r❞❡r ❧✐♠✐t
◮ ❚❤❡ ❛✈❡r❛❣❡ ❉♦❙ ❤❛s ❜❡❡♥ ❝❛❧❝✉❧❛t❡❞ ✐♥ t❤❡ ♣r❡s❡♥❝❡ ♦❢ ❛
t✉♥♥❡❧✐♥❣ ♣r♦❜❡
◮ ❚❤❡ ❝✉rr❡♥t ✐♥ ❛ t✉♥♥❡❧✐♥❣ ❡①♣❡r✐♠❡♥t ❤❛s ❜❡❡♥ st✉❞✐❡❞ ❢♦r
❛r❜✐tr❛r② ❞✐s♦r❞❡r r❡❛❧✐③❛t✐♦♥s
◮ ❚❤❡ ❛♣♣r♦❛❝❤ ✐s ✉♥✐✈❡rs❛❧ ❛♥❞ ❛♣♣❧✐❡s ❡✳❣✳ t♦ ▼❛❥♦r❛♥❛
❢❡r♠✐♦♥s ✐♥ ♥❛♥♦✇✐r❡s ✇❤✐❝❤ ❛❧s♦ ❢❛❧❧ ✐♥t♦ t❤❡ ❇ − ❉ ❝❧❛ss ✭❬❇❛❣r❡ts✱ ❆❧t❧❛♥❞ ✷✵✶✷❪✮
◮ ❉♦❙ ❞♦❡s ♥♦t ❞✐r❡❝t❧② tr❛♥s❧❛t❡ ✐♥t♦ ❝♦♥❞✉❝t❛♥❝❡ ✕ ③❡r♦✲❜✐❛s
❝♦♥❞✉❝t❛♥❝❡ ✐s q✉❛♥t✐③❡❞✱ ❧❡❛❞✐♥❣ t♦ ❛ ❞✐♣ ✐♥ ❞■/❞❱ ❛t ❱ = ✵ ✐♥ ❝❧❛ss ❉
SLIDE 22
❉❡♥s✐t② ♦❢ st❛t❡s ❛t ❤✐❣❤ ❡♥❡r❣✐❡s
❆t ❊ ≫ ❊❚❤ ✇❡ ✉s❡ ❛ ♠❡❛♥✲✜❡❧❞ ❢♦r♠✉❧❛ ρ(r, ❊) = ν ❘❡ ❝♦s θ(r, ❊) ■t ②✐❡❧❞s✱ ✐♥ ♣❛rt✐❝✉❧❛r ◆ = πν❘✷
- ✶ − (✷ −
√ ✷)
- ❊❚❤
❊
- ,
♣❧♦tt❡❞ ✐♥ ❞❛s❤❡❞ ❜❧✉❡ ♦♥ t❤❡ ❧❡❢t ✜❣✉r❡✳ ❚❤❡ r❡❞ ❝✉r✈❡ ✐s ♥✉♠❡r✐❝❛❧✳
SLIDE 23
❚♦♣♦❧♦❣✐❝❛❧ t❡r♠
❋♦r ♦✉r ♣❛r❛♠❡t❡r✐③❛t✐♦♥✱ ✐t ❡①♣❧✐❝✐t❧② r❡❛❞s ❙θ[◗] = ✐ ✹
- ❞✷r
- s✐♥ θ❢
- ∇θ❢ × ∇φ❢
- + s✐♥ ❦❢
- ∇❦❢ × ∇χ❢
- ■t ❝❛♥ ❜❡ ✇r✐tt❡♥ ✐♥✈❛r✐❛♥t❧② ❛s ❛ ❲❡ss✲❩✉♠✐♥♦✲❲✐tt❡♠ t❡r♠
❙θ[◗] = ✐ǫ❛❜❝ ✷✹π ✶
✵
❞t
- ❞✷r str
- Q−✶(∇❛Q)Q−✶(∇❜Q)Q−✶(∇❝Q)
- ✇❤❡r❡ ◗ ✐s ❡①t❡♥❞❡❞ ♦♥t♦ ❛ t❤✐r❞ ❞✐♠❡♥s✐♦♥ t✳ ❚❤❡ ✈❛r✐❛t✐♦♥
δ❙θ[◗] ♦♥❧② ❞❡♣❡♥❞s ♦♥ ◗ = Q|t=✶✳ ■❢ ◗✷ = ✶✱ t❤❡♥ δ❙θ[◗] ≡ ✵ ❡q✉❛❧s ❡①❛❝t❧② ③❡r♦✱ s♦ t❤❛t ❙θ[◗] = ❝♦♥st ♦✈❡r ❛♥② ❝♦♥♥❡❝t❡❞ ♣❛rt ♦❢ t❤❡ ♠❛♥✐❢♦❧❞✱ t❤✉s ♣❧❛②✐♥❣ t❤❡ r♦❧❡ ♦❢ ❛ t♦♣♦❧♦❣✐❝❛❧ t❡r♠✳
SLIDE 24
❚❆ =
- ✶ +
❊ ✷ − ❊ ✷
✵
✷❊Γ −✶ ❋♦r Γ ≪ ω✵ ✇❡ ❣❡t ❛t ③❡r♦ t❡♠♣❡r❛t✉r❡ ❞■ ❞❱ ∝ ρ(❡❱ )
∞
- ✵
❚❆❞❊✵ ✭✶✮ t❤✐s ✐s ❡❛s✐❧② ❣❡♥❡r❛❧✐③❡❞ t♦ ✜♥✐t❡ t❡♠♣❡r❛t✉r❡s
SLIDE 25
▼❛❥♦r❛♥❛ ❢❡r♠✐♦♥
◮ s❡❧❢✲❝♦♥❥✉❣❛t❡ ✭❤❡r♠✐t✐❛♥✮ ♣❛rt✐❝❧❡
γ† = γ,
◮ ❡♥❡r❣② ❡q✉❛❧ t♦ ❡①❛❝t❧② ③❡r♦✱ s✐♥❝❡
[❍, γ†] = ❊γ† ❛♥❞ [❍, γ] = −❊γ
◮ ❤❛❧❢ ❛ ❝♦♥✈❡♥t✐♦♥❛❧ ❢❡r♠✐♦♥
❝† = γ✶ + ✐γ✷ ❝ = γ✶ − ✐γ✷
◮ ✐❢ γ ✐s ♠❛❞❡ ♦✉t ♦❢ ❡❧❡❝tr♦♥✐❝ ♦♣❡r❛t♦rs ψ, ψ† t❤❡♥
γ = λ∗ψ† + λψ
SLIDE 26
▼❛❥♦r❛♥❛ ❢❡r♠✐♦♥ ❛♥❞ s✉♣❡r❝♦♥❞✉❝t✐✈✐t②
◮ ❡❧❡❝tr♦♥✲❤♦❧❡ ♠✐①✐♥❣ ✐s ♥❡❝❡ss❛r② ❢♦r γ✱ ❛♥❞ ✐s ♣r♦✈✐❞❡❞ ❜②
s✉♣❡r❝♦♥❞✉❝t✐✈✐t② ❍ = ❍✵ ∆ ∆∗ −Θ−✶❍✵Θ
- ✇✐t❤ t✐♠❡✲r❡✈❡rs❛❧ Θ = s②❑ ✭s② ❛❝ts ♦♥ s♣✐♥✱ ❑ ✐s ❝✳❝✳✮✱