Changes between Version 7 and Version 8 of 368sextets

Timestamp:

Oct 25, 2021, 5:18:02 PM (3 years ago)

Author:

TaylorMurphy

Comment:

--

368sextets

@@ -64 +64 @@
 \end{multline*}
 }}}
-The exotic fields can couple either to up-type quarks (//q// = //u//) or to down-type quarks (//q// = //d//). We allow for different couplings and effective cutoffs for each operator (and for each fermion-quark combination, with //I// being a quark flavor index).[[BR]]The third line contains an interesting operator coupling sextets to a quark, a gluon, and a photon or //Z// boson.
+The exotic fields can couple either to up-type quarks (//q// = //u//) or to down-type quarks (//q// = //d//).[[BR]]The sextet weak hypercharge differs in each case in order to preserve SM U(1) invariance.[[BR]]We allow for different couplings and effective cutoffs for each operator (and for each fermion-quark combination, with //I// being a quark flavor index).[[BR]]The third line contains an interesting operator coupling sextets to a quark, a gluon, and a photon or //Z// boson.
 
 The couplings in these operators are implemented as follows in the model file:
@@ -95 +95 @@
 \end{multline*}
 }}}
-In this case, simultaneous Lorentz and gauge invariance requires a SM lepton (in the absence of other exotic fields).\\
+We again have scalars coupling to both up- and down-type quarks.[[BR]]In this case, simultaneous Lorentz and gauge invariance requires a SM lepton (in the absence of other exotic fields).\\
 For full generality, these couplings are therefore in both quark and lepton generation space.