The following relations between CGLN
amplitudes and helicity
amplitudes will be used in our calculations.
(click here
for a larger image)
Further details can be found in D. Drechsel and
L. Tiator , J. Phys. G 18 (1992) 449-497 (scanned
version) (for expressions with CGLN amplitudes) and G. Knöchlein,
D. Drechsel and L. Tiator, Z. Phys. A 352 (1995) 327-343 (for expressions
with helicity amplitudes) postscript
compressed (431 kB) and nucl-th/9506029
. Channel:
K+L
K0L
K+S0
K0S+
K+S-
K0S0
Amplitudes: CGLN(F1,...,F6) Helicity(H1,...,H6) Invariant
Amplitudes(A1,...,A6)
Model input (on and
off): Born K*
(893)K1(1270)
Resonances in KL:S11(1650)P11(1710)P13(1720) D13(1900)
(missing resonance)
Resonances in KS:S11(1650)P11(1710) P13(1720) S31(1900) P31(1910)
Change
values of Born couplings, relative to standard values: gKLN
= -13.47, gKSN
= 4.25 (no factors of 4p):
gKLN
gKSN
Change values of vector
meson couplings GV,T
= ggKK*
gV,TK*YN
(relative
to standard values):
K* (893)
K1(1270)
GV
GT
GV
GT
Change values of resonance couplings
G1,2,3=
g1,2,3gNN*
gKYN (relative to
standard values):
KL
and
KS
S11(1650)
P11(1710)
P13(1720)
G1
G3
G1
G3
G1
G2
G3
KL only
KS only
D13(1900)
S31(1900)
P31(1910)
G1
G2
G3
G1
G3
G1
G3
Choose kinematical variables
choose an independent (running)
variable: Q² W QK
choose values for Q², W, QK,
step
size and maximum value: