We present a complete calculation of the contributions to the effective leptonic weak mixing angle, sin^2theta_eff, generated by closed fermion loops at the two-loop level of the electroweak interactions. This quantity is the source of the most stringent bound on the mass, M_H, of the only undiscovered particle of the Standard Model, the Higgs boson. The size of the corrections with respect to known partial results varies between -4*10^-5 and -8*10^-5 for a realistic range of M_H from 100 to 300 GeV. This translates into a shift of the predicted (from sin^2theta_eff alone) central value of M_H by +19 GeV, to be compared with the shift induced by a recent change in the measured top quark mass which amounts to +36 GeV. Our result, together wi...
We present the dominant two-loop O (G_F"2M_H"4) electroweak corrections to the fermionic d...
I discuss the importance of the O(g(4)m(t)(2)/M-w(2)) corrections to the effective electroweak angle...
The relationship between anti M anti S and pole masses of the vector bosons Z and W is calculated at...
We present a complete calculation of the contributions to the effective leptonic weak mixing angle, ...
We present a complete calculation of the contributions to the effective leptonic weak mixing angle, ...
Electroweak precision observables allow stringent tests of the Standard Model at the quantum level a...
The result for the Higgs-dependent electroweak two-loop bosonic contributions to the effective lepto...
AbstractThe result for the Higgs-dependent electroweak two-loop bosonic contributions to the effecti...
We present a calculation of the electroweak mixing parameter $\sin^2 \theta_{eff}^{lept}$ that incor...
In the Standard Model, we compute the leading two loop corrections growing like the second power of ...
AbstractWe present the complete bosonic contributions to the effective weak mixing angle, sin2θeffle...
In order to test the accuracy of the Heavy Top-mass Expansion (HTE) employed in recent two-loop calc...
The prediction of the effective electroweak mixing angle $\sin^2\theta_{\rm eff}^{\rm b}$ in the Sta...
We compute the two-loop electroweak corrections due to the top quark to the gluon fusion production ...
The relationship between MS and pole masses of the vector bosons Z and W is calculated at the two-lo...
We present the dominant two-loop O (G_F"2M_H"4) electroweak corrections to the fermionic d...
I discuss the importance of the O(g(4)m(t)(2)/M-w(2)) corrections to the effective electroweak angle...
The relationship between anti M anti S and pole masses of the vector bosons Z and W is calculated at...
We present a complete calculation of the contributions to the effective leptonic weak mixing angle, ...
We present a complete calculation of the contributions to the effective leptonic weak mixing angle, ...
Electroweak precision observables allow stringent tests of the Standard Model at the quantum level a...
The result for the Higgs-dependent electroweak two-loop bosonic contributions to the effective lepto...
AbstractThe result for the Higgs-dependent electroweak two-loop bosonic contributions to the effecti...
We present a calculation of the electroweak mixing parameter $\sin^2 \theta_{eff}^{lept}$ that incor...
In the Standard Model, we compute the leading two loop corrections growing like the second power of ...
AbstractWe present the complete bosonic contributions to the effective weak mixing angle, sin2θeffle...
In order to test the accuracy of the Heavy Top-mass Expansion (HTE) employed in recent two-loop calc...
The prediction of the effective electroweak mixing angle $\sin^2\theta_{\rm eff}^{\rm b}$ in the Sta...
We compute the two-loop electroweak corrections due to the top quark to the gluon fusion production ...
The relationship between MS and pole masses of the vector bosons Z and W is calculated at the two-lo...
We present the dominant two-loop O (G_F"2M_H"4) electroweak corrections to the fermionic d...
I discuss the importance of the O(g(4)m(t)(2)/M-w(2)) corrections to the effective electroweak angle...
The relationship between anti M anti S and pole masses of the vector bosons Z and W is calculated at...