diff --git a/HEN_HOUSE/doc/src/pirs898-egs++/common.doxy b/HEN_HOUSE/doc/src/pirs898-egs++/common.doxy
index 2e9ec134b..a2c2e4a21 100644
--- a/HEN_HOUSE/doc/src/pirs898-egs++/common.doxy
+++ b/HEN_HOUSE/doc/src/pirs898-egs++/common.doxy
@@ -309,7 +309,7 @@ The Monte Carlo transport parameters have important and significant influence on
     Electron-step algorithm        = PRESTA-II      # PRESTA-II (default),PRESTA-I
     Spin effects                   = On             # On (default),Off
     Brems angular sampling         = KM             # Simple,KM (default)
-    Brems cross sections           = BH             # BH (default),NIST
+    Brems cross sections           = BH             # BH (default), NIST, NRC
     Pair angular sampling          = Simple         # Off, Simple (default),KM
     Triplet production             = Off            # On or Off (default)
     Electron Impact Ionization     = Off            # On, Off (default), casnati, kolbenstvedt, gryzinski
diff --git a/HEN_HOUSE/interface/egs_interface2.h b/HEN_HOUSE/interface/egs_interface2.h
index 38b109a5d..6baeca119 100644
--- a/HEN_HOUSE/interface/egs_interface2.h
+++ b/HEN_HOUSE/interface/egs_interface2.h
@@ -419,12 +419,14 @@ struct EGS_XOptions {
   /*! Determines the bremsstrahlung cross sections differential in the
     photon energy to be used for sampling the photon energy.
     If set to 0, the Bethe-Heitler high energy approximation will be
-    used, if set to 1 the NIST tabulations provided by Steve Seltzer
-    will be employed. Default is 0.
+    used. If set to 1, the NIST tabulations provided by Steve Seltzer
+    will be employed. If set to 2, the NRC brems data will be used,
+    which is a modified version of the NIST data with corrected
+    electron-electron brems contributions. Default is 0.
 
     Can be set in the input file using
     \verbatim
-    Brems cross sections= BH or NIST
+    Brems cross sections= BH or NIST or NRC
     \endverbatim
   */
   EGS_I32   ibr_nist;