We compute the one-loop anomalous dimensions of the low-energy effective Lagrangian below the electroweak scale, up to terms of dimension six. The theory has 70 dimension-five and 3631 dimension-six Hermitian operators that preserve baryon and lepton number, as well as additional operators that violate baryon number and lepton number. The renormalization group equations for the quark and lepton masses and the QCD and QED gauge couplings are modified by dimension-five and dimension-six operator contributions. We compute the renormalization group equations from one insertion of dimension-five and dimension-six operators, as well as two insertions of dimension-five operators, to all terms of dimension less than or equal to six. The use of the ...
We perform a systematic study of flavor-diagonal parity- and time-reversal-violating operators of di...
We calculate the complete order y 2 and y 4 terms of the 59 × 59 one-loop anomalous dimension matrix...
We calculate the complete order y^2 and y^4 terms of the 59 x 59 one-loop anomalous dimension matrix...
Abstract The gauge-invariant operators up to dimension six in the low-energy effective field theory ...
We calculate the gauge terms of the one-loop anomalous dimension matrix for the dimension-six operat...
The one-loop renormalization group equations for the Standard Model (SM) Effective Field Theory (EFT...
Abstract We showed in a previous publication that there are six independent dimension-seven operator...
We calculate the one-loop anomalous dimension matrix for the dimension-six baryon number violating o...
AbstractWe calculate the one-loop anomalous dimension matrix for the dimension-six baryon number vio...
We extend the low-energy effective field theory relevant for b → s transitions up to operators of ma...
Abstract We obtain the complete operator bases at mass dimensions 5, 6, 7, 8, 9 for the low energy e...
We calculate the gauge terms of the one-loop anomalous dimension matrix for the dimension-six operat...
Abstract General analyses of B-physics processes beyond the Standard Model require accounting for op...
We perform a systematic study of flavor-diagonal parity- and time-reversal-violating op-erators of d...
We compute the one-loop renormalisation group running of the bosonic Standard Model effective opera...
We perform a systematic study of flavor-diagonal parity- and time-reversal-violating operators of di...
We calculate the complete order y 2 and y 4 terms of the 59 × 59 one-loop anomalous dimension matrix...
We calculate the complete order y^2 and y^4 terms of the 59 x 59 one-loop anomalous dimension matrix...
Abstract The gauge-invariant operators up to dimension six in the low-energy effective field theory ...
We calculate the gauge terms of the one-loop anomalous dimension matrix for the dimension-six operat...
The one-loop renormalization group equations for the Standard Model (SM) Effective Field Theory (EFT...
Abstract We showed in a previous publication that there are six independent dimension-seven operator...
We calculate the one-loop anomalous dimension matrix for the dimension-six baryon number violating o...
AbstractWe calculate the one-loop anomalous dimension matrix for the dimension-six baryon number vio...
We extend the low-energy effective field theory relevant for b → s transitions up to operators of ma...
Abstract We obtain the complete operator bases at mass dimensions 5, 6, 7, 8, 9 for the low energy e...
We calculate the gauge terms of the one-loop anomalous dimension matrix for the dimension-six operat...
Abstract General analyses of B-physics processes beyond the Standard Model require accounting for op...
We perform a systematic study of flavor-diagonal parity- and time-reversal-violating op-erators of d...
We compute the one-loop renormalisation group running of the bosonic Standard Model effective opera...
We perform a systematic study of flavor-diagonal parity- and time-reversal-violating operators of di...
We calculate the complete order y 2 and y 4 terms of the 59 × 59 one-loop anomalous dimension matrix...
We calculate the complete order y^2 and y^4 terms of the 59 x 59 one-loop anomalous dimension matrix...