TFPT scientific source excerpt Original repository path: experiments/theory-contracts/source-dynamics-selection-20260920/PROOF.txt Original file SHA-256: 03c09468b07cc68abd31d7f8d6715dd474564728d053ccb063a67a1ca71c89d2 Inclusive original lines: 30-58 Line numbers below refer to the original source. This bounded excerpt is source evidence; it is not a new proof/checker run. Conversation metadata and personal execution details are omitted where indicated. 000030 | We test the ALREADY CONDITIONAL ten-channel edge: 000031 | Gamma=Z^10, K=diag(1^9,-1), B(x,y)=x^T K y, 000032 | V_x=cocycle_x :exp(i x^T K phi):, 000033 | q(x)=sum x_i, 000034 | Y=(-1/3,-1/3,-1/3,1/2,1/2,0,0,0,1,1), 000035 | g=(2,2,2,2,2,0,0,0,3,3) modulo4, 000036 | n=(1,1,1,-1,-1,-1,-1,-1,-1,3), z=e9-e10. 000037 | Write a=(1,1,1,-1,-1,-1,-1,-1), m=(a,0,3)=n+e9. 000038 | The previous selected energy is V_aux=K+2Kmm^T K. 000039 | Equal original free velocities are normalized to one: V0=I. 000040 | Neither this granted ten-channel comparison nor its interaction is a new 000041 | derivation from the one-copy QWZ source or from P1/P2. 000042 | 000043 | 1. An energy-preserving dictionary is different from changing the energy 000044 | 000045 | Use the existing integral unimodular W=W_aux, with 000046 | W^T K W=G_E8 direct_sum diag(1,-1). 000047 | If phi=W chi, a passive change of fields necessarily gives 000048 | K'=W^T K W, V'=W^T V W. (2) 000049 | For V0 the second matrix is W^T W, not G_E8 direct_sum I2. 000050 | The latter is W^T V_aux W. Replacing one with the other changes the 000051 | physical Hamiltonian and its state/correlation dynamics. 000052 | 000053 | For the specific positive generalized metrics used here, V K V=K and 000054 | K^2=I. The equal-time covariance metric is K V^-1 K=V. Consequently the 000055 | scaling dimension of V_x is Delta_V(x)=x^T V x/2. This formula is NOT 000056 | asserted for an arbitrary positive kinetic matrix. Alternatively the 000057 | dimensions below follow by diagonalizing to the declared free chiral 000058 | coordinates and using the transported vertex charges.