Science is a wonderful thing if one doesn't have to earn one's living on it... [A.Einstein]
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Beyond Standard Model I (NJSF139) course exercise sheets   
Exercise sheet 1: Chiral anomaly and gauge dependence cancellation in the SM
The merit of this exercise is to take a look at a typical one-loop SM amplitude and study its xi-dependence (within the class of t'Hooft's "renormalizable gauges") in the absence and presence of anomaly in the axial vector currents.
Exercise sheet 2: Gauge coupling evolution in Yang-Mills theories - part I
Here you have to regularize a number of two-point Green's functions in a general Yang-Mills theory coupled to formions and scalars and determine the coefficient of the UV poles therein.
Exercise sheet 3: Gauge coupling evolution in Yang-Mills theories - part II
Here you do the same as in the previous exercise, this time for the three-point functions. With all that information at hand you can finally derive the infamous prescription for the general form of the one-loop gauge beta-function in Yang-Mills and dream about the Nobel prize you'd get if only you did the calculation 50 years ago.
Exercise sheet 4: Neutrinoless double beta decay leptonic matrix element
In this exercise your task is to derive and depict the bands in wich you can find the value of the weak part of the matrix element for the neutrinoless double-beta decay process as a function of the mass of the lightest (Majorana) neutrino in the simple seesaw scenario we have discussed so far. You are supposed to analyze both the normal as well as the inverse hierarchy settings taking into accounts the existing uncertainties in the PMNS mixing angles and CP phases.
Exercise sheet 5: Scalar sector of the type-II seesaw model
In this exercise you will analyze the scalar sector of the type-II seesaw model with a heavy SU(2)_L triplet, calculate its induced VEV in terms of the electroweak one and estimate its impact on the value of the SM rho parameter. This, in turn, provides an upper limit on the triplet VEV.
Lecture notes   
Notes ver. 1
This is the first (and very incomplete) version of the lecture notes.
Nobel prize in physics 2015
This is a supplementary material including a brief introduction into neutrino oscillations and the main experiments which contributed to their discovery. (in Czech)
Supplementary material   
Leptogenesis: A Pedagogical Introduction by Y. Nir
Great lecture notes on leptogenesis containing a detailed derivation of the Davidson-Ibarra limit from the formula we have obtained in the lecture.
Lecture videos    here
Lecture 1
QED versus the four-fermion description of weak interactions, the model with W, parity violation and the need for Z, tree unitarity principle, "shifted" scalar.
Lecture 2
Why would one formulate a theory in terms of a shifted scalar, symmetric vs. asymmetric vacuum, Goldstone theorem and the Higgs trick, Unitary gauge and the vector boson propagator asymptotics.
Lecture 3
Renormalizable gauges, xi-independence of measurable quantities (comments on Exercise sheet 1), the abelian Higgs model in the R-xi gauges, the Goldstone propagator, the t'Hooft-Feynman gauge. Running coupling in phi^4 theory and the concept of renormalization group (+ comments on Exercise sheets 2 and 3).
Lecture 4
Naive and anomalous Ward identities, general chiral transformation, Fujikawa form of the anomalous contribution to the lagrangian density, anomalous terms associated with global chiral transformations and their innocence in the perturbative approach, anomalies associated to local transformations and their potentially fatal impact on the gauge invariance of amplitudes. Pions as Goldstone modes of the spontaneously broken flavor symmetry of QCD.
Lecture 5
The three three-fold unitary symmetries of 3-flavor QCD, spontaneous breaking of the SU(3)_A x U(1)_A global symmetry by the QCD condensate, QCD phase transition, classification of hadrons in terms of SU(3)_f and U(1)_B, pions as Goldstone modes of SU(2)_V. Effective neutral pion decay lagrangian - the naive version - and its pathologies, anomaly matching and the anomaly-induced neutral pion decay lagrangian.
Lecture 6
Local anomalies in the SM - (hyper)charge quantization, neutrality of neutrons. Evidence of non-zero neutrino masses: neutrino flavor oscillations. Adding a RH neutrino to the SM, Dirac mass, smallness of Dirac neutrino Yukawa couplings. SM hypercharge dequantization with Dirac neutrinos.
Lecture 7
B and L as accidental global anomalous symmetries in the SM. Gaugeability of B-L and its relation with hypercharge dequantization in the Dirac neutrino case. Smallness of Yukawa couplings. Majorana fermions.
Lecture 8
Majorana fermions II. Majorana mass term for the RH neutrino, its natural size, seesaw mechanism, light and heavy Majorana neutrinos. Hypercharge quantization restoration in the SM extension with massive Majorana neutrinos.
Lecture 9
Anatomy of the type-I seesaw formula, symmetry of the Majorana neutrino mass matrix, large new physics scale. Indication of a large new physics scale from the gauge couplings' evolution in the Standard Model.
Lecture 10 Flavour aspects of models with Majorana neutrinos. Rare processes featuring lepton flavor violation (e.g., mu to e+photon). CP violation in models with Majorana neutrinos.
Lecture 11
Perturbative lepton number violation in the seesaw model, neutrinoless double-beta decay. Baryon number problem of the Standard Model (the fate of baryons in the early Universe).
Lecture 12
Early Universe baryon chemistry, neutron to proton number density ratio evolution (neutrino decoupling, deuterium bottleneck), nucleosynthesis. Primordial deuterium abundance as a tool to measure baryon to photon number density ratio. B-symmetric initial conditions and the 9-orders of magnitude failure of the SM. Asymmetric initial state? Sacharov's conditions for baryogenesis. Baryogenesis failure in the SM.
Lecture 13
Baryogenesis through leptogenesis in the seesaw model, Cassas-Ibarra parametrization, Davidson-Ibarra limit on the mass of the lightest RH neutrino.
Lecture 14
Dimension 5 Weinberg's operator as an effective low-energy description of a high-scale RH neutrino dynamics. Alternative "openings" of the Weinberg's operator. Type-II and type-III seesaw models and their salient features.

Success is not final, failure is not fatal: it is the courage to continue that counts. [W.Churchill]
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