********* Eigenvalues for the 2+1 transverse lattice  *********
Couplings:  m^2, G^2 N, la_1, la_2, la_3, tau_1, tau_2
             0      1     2     3     4      5      6  
Use chi^2 fit with 13 criteria, and tolerance 0.001.  
Overall scale from minimizing chi^2.
2 parity doublets with fractional errors 2 0.5.
Spectrum for P_perp a = (0)  ( 0.25) 
 using (# states, o, multiplet, c^2 error for each) =
  (4, 1 & -1, 1 & 2, 0.5 2 0.5 0.5)
  (4, 1 & -1, 2 & 1, 0.5 0.5 0.5 0.5).
Spectra extrapolated using (K,p) = (18/2,6)  (18/2,8) 
  (20/2,6)  (20/2,8)  (24/2,6)  (32/2,6) .
Winding potential using (n,K,p) = ( 2,20/2,4)  ( 2,20/2,6) 
  ( 2,24/2,4)  ( 2,28/2,4)  ( 3,21/2,5)  ( 3,21/2,7)  ( 3,23/2,5) 
  ( 3,27/2,5)  ( 4,20/2,6)  ( 4,20/2,8)  ( 4,22/2,6)  ( 4,26/2,6) .
Heavy potential determined using (n,K,p,K_max) = ( 1,-32/2,2,4) 
  ( 1,-32/2,4,4)  ( 1,-32/2,2,5)  ( 1,-34/2,2,4)  ( 1,-44/2,2,5) 
  ( 1,-60/2,2,4) ,
 L = 3 4 6 (all in G^2 N units); relative scale error 0.25.
Roundness determined using (n,K,p,K_max) = ( 1,-19/2,3,4) 
  ( 1,-19/2,5,4)  ( 1,-19/2,3,5)  ( 1,-33/2,3,4)  ( 1,-33/2,3,5) 
  ( 1,-49/2,3,4) 
 L=3 and error 0.3; 
  ( 1,-19/2,3,4)  ( 1,-19/2,5,4)  ( 1,-19/2,3,5)  ( 1,-33/2,3,4) 
  ( 1,-33/2,3,5)  ( 1,-49/2,3,4) 
 L=1 and error 0.3; all in G^2 N units.
p-extrapolation using n=( 1) and (K,p) = (21/2,3)  (27/2,3) 
  (39/2,3)  (21/2,5)  (27/2,5)  (21/2,7)  (23/2,7) .
Result format:
 fit info, # steps, chi^2, p damping, and scale g^2 N/(a sigma);
 the 7 couplings (G^2 N units) and which--if any--were fit;
 winding and longitudinal string tension fits;
 Roundness with calculated and derived values (G^2 N units);
 the rescaled spectrum for each P_perp*a and c^2 values.

2 66 7.299773 -0.726934 12.776293
0.032492 1.000000 0.903877 -0.250713 3.703849 3.314327 -2.983549  2 3 4 5 6
0.127818 -1.127144 1.788795  0.080222 -0.218331 0.498032
0.267022 0.311201  0.389286 0.263290  
 35.271936 35.332125 1.572649
 49.081673 49.126564 1.172947
 79.171367 79.199314 0.730214
 93.269061 93.305290 0.946614
 26.485239 26.509787 0.641409
 75.128206 75.159083 0.806753
 100.754546 100.768109 0.354368
 103.235478 103.239898 0.115470