HQET parameters and their covariance matrices
as described in appendix C of 
HQET at order 1/m: I. Non-perturbative parameters 
in the quenched approximation

files:

param_mb.dat
param_mb_castat=0.dat
para_fB.dat
para_fB_castat=0.dat
corr_mb.dat
corr_mb_castat=0.dat
corr_fB.dat
corr_fB_castat=0.dat
-----------------------------------------------------


para_mb.dat
------------

contains the set "a" of HQET parameters, needed 
for a computation of the b-quark mass.

The parameters are 

omega_1^{stat} = mbare^{stat}
omega_1^{1/m}  = mbare^{1/m}
omega_4        = omega_kin


and they are given for the different actions, quark masses, 
and lattice spacings, labeled by an index alpha as explained 
in the paper (eq. C.2)
The theta angles have been fixed to their standard values.



corr_mb.dat
-----------

The covariance matrix C^a_{alpha beta} of the set "a",
with the convention that alpha < beta and that alpha is
the inner index



para_fB.dat
-----------

The set "b" of parameters, needed for a computation of 
heavy-light decay constant. 

omega_2^{stat} =  lnZ_A^{stat}
omega_2^{1/m}  =  lnZ_A^{1/m}
omega_3^{1/m}  =  cA^(1) 
omega_4        =  omega_kin 
omega_5        =  omega_spin

are given for the different actions and lattice spacings, 
labeled by an index alpha (following eq. C.3)
In that case the quark mass has been fixed to the interpolated
value, though a matching of the spin-averaged meson mass.
Again the theta angles are fixed to their standard values.


corr_fB.dat
-----------

The covariance matrix C^b{alpha beta} of the set "b", 
with the convention that alpha < beta and that alpha is
the inner index



The computation has been repeated with cA^{stat} fixed to 0
(instead of its one-loop value). 
The results can be found in the files ..._castat=0 ,
which are written with the same structure.