diff --git a/qma_coulomb_hardness_v2.txt b/qma_coulomb_hardness_v2.txt
index 67d9c8a..ec42008 100644
--- a/qma_coulomb_hardness_v2.txt
+++ b/qma_coulomb_hardness_v2.txt
@@ -747,11 +747,7 @@ tail bound exp(-|r|) of phi it satisfies, for some absolute C,
 
     c (1+d)^{-C} e^{-d}  <=  T(d)  <=  C (1+d)^{C} e^{-d} .         (26)
 
-The hopping to be supplied by the continuum. The cubature replacement shows that the real
-continuum orbital matrix, evaluated on the orbitals centered at u_i, has
-hopping entries t_e = lambda T(|u_i - u_j|) in the units of H_d, up to an
-error of order p(n,D) lambda^{-0.1}. So to realize the target t_e^tar of
-(23), one must choose each link length d_e so that
+The hopping to be supplied by the continuum. The real continuum orbital matrix, evaluated on the orbitals centered at u_i, has hopping entries t_e = lambda T(|u_i - u_j|) in the units of H_d, up to an error of order p(n,D) lambda^{-0.1}. So to realize the target t_e^tar of (23), one must choose each link length d_e so that
 
     lambda T(d_e) = tau sqrt( K_e (U - v(d_e)) ) .                 (27)