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Googlism comments
c_c is fully faithful left
c_c is 10%
c_c is insufficient to describe the data
c_c is important
c_c is most serious and affected largely by the ambiguous radiative correction
c_c is larger than that of flfl
c_c is then processed at high temperature
c_c is shown in fig
c_c is an external input
c_c is a singlet state
c_c is unobservable
c_c is larger
c_c is in a colour singlet state
c_c is small
c_c is produced in electron
c_c is completely determined if themomenta of one incoming and one outgoing particle
c_c is found to be insufficient to describe the data
c_c is the leading
c_c is the centre of mass energy of the
c_c is formed until the j/ exits the
c_c is formed in a color neutral state and later becomes the color
c_c is an especially clear case
c_c is assigned to the
c_c is represented in the form
c_c is given by c
c_c is tiny
c_c is also fairly stiff
c_c is negligible
c_c is estimated from
c_c is proportional to cos ff/ sin fi
c_c is select em
c_c is readily obtained from that for gg
c_c is taken into account
c_c is drawn in three different ways
c_c is the compression of the core
c_c is
c_c is produced in
c_c is in a colour octet configuration
c_c is 0
c_c is dense in l_p
c_c is proportional to cos ff= sin fi
c_c is an integer and _ r_e_ a_d also returns information in the parameter
c_c is negative
c_c is suppressed by boltzmann factor
c_c is not observable
c_c is excluded by the observed j=
c_c is most serious and affected largely by an ambiguous radiative correction
Nickname c_c
- c_c (Points: 0)