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 New theories ofways to quantizetechniques in (super) Yang−Millsgravitystrings

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 E=p²/2m E=mc² p=mdx/ds p²+m²=0 δS/δφ=0 S=∫dτ ½(vm²-v⁻¹ẋ²) -ds²=dxᵘdxᵛgᵤᵥ 〈gᵤᵥ〉=ηᵤᵥ/κ² Rᵤᵥ-½gᵤᵥ=2Tᵤᵥ [p,q]=-i (i∂/∂t-H)ψ=0 (p̸-m)ψ=0 〈f|i〉=∫Dp Dq exp(-iS) Δ=-i/½(p²+m²-iε) dσ/dt=½(2π)³|T|²/λ² ∇'=eⁱᵠ∇e⁻ⁱᵠ [∇ᵤ,∇ᵥ]=iFᵤᵥ Q²=0 pᵦᵦ̇=λᵦλ̄ᵦ̇ A=gⁿ⁻²〈ij〉⁴/〈12〉...〈n1〉 M²=μ²exp(-1/g²) {q,q̄}=2p̸ δθ=ε, δx=iεΓθ L=-¼R+ψ̄ᵣγʳᵘᵛ∇ᵤψᵥ S=(1/2πα')∫d²σ(∂X)² A=g²B[-α(s),-α(t)] J=α'M²+α₀ Z=〈exp(∫φO)〉 E=p²/2m E=mc² p=mdx/ds p²+m²=0 δS/δφ=0 S=∫dτ ½(vm²-v⁻¹ẋ²) -ds²=dxᵘdxᵛgᵤᵥ 〈gᵤᵥ〉=ηᵤᵥ/κ² Rᵤᵥ-½gᵤᵥ=2Tᵤᵥ [p,q]=-i (i∂/∂t-H)ψ=0 (p̸-m)ψ=0 〈f|i〉=∫Dp Dq exp(-iS) Δ=-i/½(p²+m²-iε) dσ/dt=½(2π)³|T|²/λ² ∇'=eⁱᵠ∇e⁻ⁱᵠ [∇ᵤ,∇ᵥ]=iFᵤᵥ Q²=0 pᵦᵦ̇=λᵦλ̄ᵦ̇ A=gⁿ⁻²〈ij〉⁴/〈12〉...〈n1〉 M²=μ²exp(-1/g²) {q,q̄}=2p̸ δθ=ε, δx=iεΓθ L=-¼R+ψ̄ᵣγʳᵘᵛ∇ᵤψᵥ S=(1/2πα')∫d²σ(∂X)² A=g²B[-α(s),-α(t)] J=α'M²+α₀ Z=〈exp(∫φO)〉 E=p²/2m E=mc² p=mdx/ds p²+m²=0 δS/δφ=0 S=∫dτ ½(vm²-v⁻¹ẋ²) -ds²=dxᵘdxᵛgᵤᵥ 〈gᵤᵥ〉=ηᵤᵥ/κ² Rᵤᵥ-½gᵤᵥ=2Tᵤᵥ [p,q]=-i (i∂/∂t-H)ψ=0 (p̸-m)ψ=0 〈f|i〉=∫Dp Dq exp(-iS) Δ=-i/½(p²+m²-iε) dσ/dt=½(2π)³|T|²/λ² ∇'=eⁱᵠ∇e⁻ⁱᵠ [∇ᵤ,∇ᵥ]=iFᵤᵥ Q²=0 pᵦᵦ̇=λᵦλ̄ᵦ̇ A=gⁿ⁻²〈ij〉⁴/〈12〉...〈n1〉 M²=μ²exp(-1/g²) {q,q̄}=2p̸ δθ=ε, δx=iεΓθ L=-¼R+ψ̄ᵣγʳᵘᵛ∇ᵤψᵥ S=(1/2πα')∫d²σ(∂X)² A=g²B[-α(s),-α(t)] J=α'M²+α₀ Z=〈exp(∫φO)〉 E=p²/2m E=mc² p=mdx/ds p²+m²=0 δS/δφ=0 S=∫dτ ½(vm²-v⁻¹ẋ²) -ds²=dxᵘdxᵛgᵤᵥ 〈gᵤᵥ〉=ηᵤᵥ/κ² Rᵤᵥ-½gᵤᵥ=2Tᵤᵥ [p,q]=-i (i∂/∂t-H)ψ=0 (p̸-m)ψ=0 〈f|i〉=∫Dp Dq exp(-iS) Δ=-i/½(p²+m²-iε) dσ/dt=½(2π)³|T|²/λ² ∇'=eⁱᵠ∇e⁻ⁱᵠ [∇ᵤ,∇ᵥ]=iFᵤᵥ Q²=0 pᵦᵦ̇=λᵦλ̄ᵦ̇ A=gⁿ⁻²〈ij〉⁴/〈12〉...〈n1〉 M²=μ²exp(-1/g²) {q,q̄}=2p̸ δθ=ε, δx=iεΓθ L=-¼R+ψ̄ᵣγʳᵘᵛ∇ᵤψᵥ S=(1/2πα')∫d²σ(∂X)² A=g²B[-α(s),-α(t)] J=α'M²+α₀ Z=〈exp(∫φO)〉