The parity-non-conserving (pnc) asymmetry in (n) over right arrow + p --> d
+ gamma at thermal energies has recently been calculated using effective f
ield-theory methods. A comparison of this calculation with much more elabor
ate calculations performed in the 70's is made. This allows one to assess t
he validity of this new approach as presently used. It is found to overshoo
t the almost exact calculations by a factor close to 1.6 (a factor 2 when o
nly the contribution involving the S-3(1) component of both the initial and
final states is retained). This discrepancy is analyzed and found to origi
nate from the over-simplified description of the deuteron and capture state
s which underlies the new approach. The claim that earlier determinations o
f the sign would be in error is also examined. It is found that the sign di
screpancy is most probably due, instead, to the fact that the pion-nucleon
interaction referred to by the authors corresponds to a parity-non-conservi
ng potential with a sign opposite to what is currently used in the field. S
ome estimates and constraints relative to the pnc pi NN coupling, h(pi)(1),
which the above asymmetry is dependent on, are reviewed. (C) 2001 Elsevier
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