.2 ρ dv dt = ρk grad p + 3 η grad (divv) + η 2 v.3 divh = 0, rote + c H t = 0 dive = ρ, H = 0, E = ρ, roth c E t = c ρv E + H c t = 0 H c E t = c ρv T

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1 NHK ( ) ( ) ( ) ( ) I. ( ν R n 2 ) m 2 n m, R = e 2 8πε 0 hca B = m ( ν = ) λ a B = 4πε 0ħ 2 m e e 2 = m

2 .2 ρ dv dt = ρk grad p + 3 η grad (divv) + η 2 v.3 divh = 0, rote + c H t = 0 dive = ρ, H = 0, E = ρ, roth c E t = c ρv E + H c t = 0 H c E t = c ρv Theory of Everything: 2 CERN L = ψi ψ g ψbψ 4 Bµν B µν g 2 ψwψ 4 Wµν W µν g 3 ψgψ 4 Gµν G µν + ψ i y ij ψ j ϕ + h.c. + D µ ϕ 2 V (ϕ) 2

3 2. ψı ψ e: ν: u: ( ) d: ( ) 2.. i t ψ = 2 2m x 2 ψ 2..2 x 2 + y 2 = r y = px + nq, n Z (x a) 2 + (y b) 2 = x 2 + y 2 2ax 2by + a 2 + b 2 3

4 (t) (x 2 ) i t ψ = 2 2m x 2 ψ + v m x t ψ ħ =, c = iγ t ψ + i γ x ψ = mψ (iγ µ µ m) ψ (x) = 0, µ = 0,, 2, 3 µ x µ, ψ (x) = ψ (x) ψ 2 (x) ψ 3 (x). ψ 4 (x) ( ) γ µ 0 σ µ ) ) =, σ µ = (Î, ˆσj, σ µ = (Î, ˆσj σ µ 0 {γ µ, γ ν } γ µ γ ν + γ ν γ µ = 2η µν, η µν = g µν magnetic moment 4

5 L = ψi ψ ψmψ 2.2 g ψbψ 4 Bµν B µν g 2 ψwψ 4 Wµν W µν g 3 ψgψ 4 Gµν G µν + ψ i y ij ψ j ϕ + h.c. + D µ ϕ 2 V (ϕ) h.c.: there are additional terms which are the hermitian conjugate of the terms that have already been written 4 F µν F µν 5

6 2.2. L = ψi ψ ψmψ g ψaψ 4 F µν F µν (930) 948 (948) = =

7 L = ψi ψ ψmψ g ψaψ 4 F µν F µν { } 950 P N +e MeV 939.6MeV P = (udd), N = (uud) u: d: (954) L = 4 f µν f µν ψγ µ ( µ iϵτ b µ )ψ m ψψ. 7

8 L = ψi ψ ψmψ g ψbψ 4 Bµν B µν g 2 ψwψ 4 Wµν W µν g 3 ψgψ 4 Gµν G µν 8

9 II NY (957) β (e, ν, u, d) ψmψ e iβ ψl Mψ R + e iβ ψr Mψ L 9

10 960 (96) g 3 ψgψ g 3 (ūgu + dgd) u d m = 0 m = 0 m 0 0

11 u R u R + u L u L u R + u L dr + d L d R + d L g 2 ψwψ 960 W Z

12 W + W Z 979 (964) 203/0/8 CERN (967) 983 CERN W Z 2

13 3

14 III DAS WAHRE IST GOTTHNLICH U = M r ( J 2 R 2 3 cos 2 θ r 2 2 ) 3 ˆ Z = [DA] [Dψ] [Dϕ] [ ˆ [ exp i d 4 x 4 F µν F µν + ( i ψdψ + h.c. ) ]] + (ψ i y ij ψ j ϕ + h.c) + D µ ϕ 2 V (ϕ) 3. ˆ Z = ˆ [DA] [Dψ] [Dϕ] exp[i d 4 x 3.2 [ 4 F µν F µν + ( i ψdψ + h.c. ) ] + (ψ i y ij ψ j ϕ + h.c) + D µ ϕ 2 V (ϕ) 4

15 4 R µν 2 g µνr = κt µν }{{}}{{} µ, ν : R µν : g µν : R : κ : T µν : 4. ( ds 2 = 2GM ) rc 2 dt 2 + dr 2 2GM rc r ( dθ 2 + sin 2 θ dϕ 2) R αβγδ R αβγδ = 48G2 M 2 c 4 r 6 D istortion r 3 D : r : D istortion = 0 3 = 5

16 4.2 ˆ Z = [Dg] [DA] [Dψ] [Dϕ] [ ˆ exp i d 4 x [ g 2κ R 4 F µν F µν + ( i ψdψ + h.c. ) ]] + (ψ i y ij ψ j ϕ + h.c) + D µ ϕ 2 V (ϕ) ˆ i d 4 x [ g 2κ R 4 F µν F µν + ( i ψdψ + h.c. ) ] + (ψ i y ij ψ j ϕ + h.c) + D µ ϕ 2 V (ϕ) 0 = (936) 6

17 (974) ˆ d 2 σ h h αβ α X µ β X µ 2π M gravity r 2 0 r = 0 5 CALTEC ˆ Z = [ [Dg] [DA] [Dψ] [Dϕ] exp ˆ d 2 σ h [ h αβ α X µ β X µ i 2π ψ µ ρ α ] ] α ψ µ M ψ (σ, µ τ) = d µ ne in(τ σ) 2 n Z 7

18 L m = α µ 2 n mα µn + 4 n Z r G r = n Z α µ nψ µr n [L m, L n ] = (m n)l m+n + {G r, G s } = 2L r+s + c 2 (4r2 [L m, G r ] = m 2r G m+r 2 ˆ Z = { [Dg] [DX] [Dψ] exp ˆ d 2 σ h [ h αβ α X µ β X µ i 2π ψ µ ρ α ] } α ψ µ M 8

19 IV S = ˆ d 2 σ { α X µ α X µ i 2π ψ µ ρ α } α ψ µ M m = 0(const.) 4(dimension) m = = 0 (D = {t, x, y, z}) (D = 0) D = 9

20 δs = ˆ 2κ 2 d D x ( G) 2 e 2Φ 0 [ α ( δg µν β G µν + δb µν β B µν + 2δΦ ) (β 2 Gµν G δg ω µν ω 4β Φ)] ˆ Z = [Dg] [DA] [Dψ] [Dϕ] ˆ exp{i d 4 x g [ 2κ R + D µϕ 2 24κ e ϕ F µνρ F µνρ 4κ λγ µ D µ λ 4 F µνf µν 4 2κ χ µγ ν γ µ λ ν ϕ + 24 g 2 tr ( ψλ ρστ ψ ) 2 2g 2 e 2 ϕ tr 24κ χ µγ µνρ D ν χ ρ ( 2 ϕ + 8 ϕ2 48 ϕ3 + ) + ( i ψdψ + h.c. ) [ χ 96κ e 2 ϕ [µ γ µ γ ρστ γ ν γχ ν] ] 2 χ µ γ ρστ γ µ λ ) ( + 8 ϕ2 48 ϕ3 + F ρστ + (ψ i y ij ψ j ϕ + h.c) [( χ µ γ ρσ γ µ ψ ) ] λγ ρσ ψ F ρσ + ]} 2 F ρστ n = 496 (perfect number) 496 = n S n S n 2 n 2 20

21 THE THEORY OF EVERYTHING (a Bohr 0 24 = m) D ˆ d 2 σ h [ h αβ α X µ β X µ i 2π ψ µ ρ α ] α ψ µ M +iµ ρ ˆ ρ+ [ Tr exp (2πα F 2 + B 2 ) ] C 2

22 S = 4G A QH Q 2 F = 2π 2 M = K3 [ 2 Q 2 +] F S [ +] 2 Q2 F L 0 = 2 (H P ) = 0 c = 6k, L 0 = n, n d(n, l) exp ( 2π nc6 ) ( ) c = 6 2 Q2 F + n = Q H ( ) 2 S = ln d (Q F, Q H ) 2π Q H Q2F + QH Q 2 F 2π LIGO VLA CERN 22

23 M M Theory M

1 (Berry,1975) 2-6 p (S πr 2 )p πr 2 p 2πRγ p p = 2γ R (2.5).1-1 : : : : ( ).2 α, β α, β () X S = X X α X β (.1) 1 2

1 (Berry,1975) 2-6 p (S πr 2 )p πr 2 p 2πRγ p p = 2γ R (2.5).1-1 : : : : ( ).2 α, β α, β () X S = X X α X β (.1) 1 2 2005 9/8-11 2 2.2 ( 2-5) γ ( ) γ cos θ 2πr πρhr 2 g h = 2γ cos θ ρgr (2.1) γ = ρgrh (2.2) 2 cos θ θ cos θ = 1 (2.2) γ = 1 ρgrh (2.) 2 2. p p ρgh p ( ) p p = p ρgh (2.) h p p = 2γ r 1 1 (Berry,1975) 2-6