Phenomenology of neutron oscillations

Volume

96B, number

PHYSICS

3,4

A. Hosoya, Duality for the Lorentz force in loop space, Phys. Lett. 92B (1980) 331.

LETTERS

3 November

1980

B.G. Konopelchenko, On the structure of the commutative Z, graded algebra’valued integrable equations, Phys. Lett. 95B (1980) 83.

Eq. (3”) should be replaced by

~*F,(m 6xqs’)

+ fqs- s’)[*F,(x(s)>,F,(x(s’))] = 0. *

+

%

The following corrections apply: (i) In formula (7) replace Vin)

(-C-J) by

F;+““‘(t-1.

(ii) In formula (20) replace R.N. Mohapatra and R.E. Marshak, Phenomenology of neutron oscillations, Phys. Lett. 94B (1980) 183. Eq. (12) should read p5(t) e 2e2 [ 1 - cos aMt] . Eq. (13) should read

(Pj&

Eq. (14) should read

&Jt) ” (&7#. *

*

‘v 282.

*

T. Chandramohan and L. Clavelli, Second order QCD contributions to thrust and spherocity, Phys. Lett. 94B (1980) 409. The correct c$ contributions to spherocity and thrust are a factor of 3 smaller than the “c~: term” shown in figs. 1 and 2. These second order contributions still dominate over the first order QCD predictions in the boundary region.

444

TG +(j,)(+,)

by

Ti+(inj(_Wj).

(iii) In formula (8) replace Z, by 21; mula (12)1, by 2Iz, where

and in for-

I,-fdf =- s= dyf(y)> l,'f d=fj @f(y). -cc

X

Therefore the sentence following formula (12) and footnote 2 are not correct. All other equations and results of this paper remain unchanged. *

*

*