Documentation fixes. This commit is targeted for a 0.924 release.

NEWS

@@ -22,7 +22,7 @@ Improvements to the ode_iv_solve_grid class.
 
 Improved error handling for calculator class.
 
-Created functions vector_refine(), file_exists(), o2isfinite(), 
+Created functions vector_refine(), file_exists(), and o2isfinite().
 
 Created classes inte_tanh_sinh_boost, inte_sinh_sinh_boost,
 inte_kronrod_boost, inte_exp_tanh_boost, nucmass_gen, and frib_mex.
@@ -35,7 +35,7 @@ vector_spec() and mult_vector_spec().
 
 Improved tabulate option for tov_love::calc_y().
 
-Updated constants to CODATA 2018 release.
+Updated constants for CODATA 2018 release.
 
 ------------------------------------------------------------------------
 Notes for 0.923 release:

src/inte/inte_kronrod_gsl.h

@@ -602,7 +602,7 @@ namespace o2scl {
       - 6: 61-point rule
       Any value other than 1-6 forces the error handler to be
       called. All classes default to the 15-point rule,
-      except for \ref inte_qags_gsl which defaults to
+      except for \ref o2scl::inte_qags_gsl which defaults to
       the 21-point rule for singularities. 
 
       The integration coefficients for use with this class and

src/inte/inte_qagil_gsl.h

@@ -42,7 +42,7 @@ namespace o2scl {
       \int_{-\infty}^b f(x)~dx =
       \int_0^1 f(b - (1-t)/t)t^{-2}~dt,
       \f]
-      and the right hand side is evaluated with \ref inte_qags_gsl.
+      and the right hand side is evaluated with \ref o2scl::inte_qags_gsl.
 
       See \ref gslinte_subsect in the User's guide for general
       information about the GSL integration classes.

src/inte/inte_qagiu_gsl.h

@@ -42,7 +42,7 @@ namespace o2scl {
       \int_a^{\infty} f(x)~dx =
       \int_0^1 f(a + (1-t)/t)t^{-2}~dt,
       \f]
-      and the right hand side is evaluated with \ref inte_qags_gsl.
+      and the right hand side is evaluated with \ref o2scl::inte_qags_gsl.
 
       See \ref gslinte_subsect in the User's guide for general
       information about the GSL integration classes.

src/inte/inte_qawo_gsl.h

@@ -42,10 +42,10 @@ namespace o2scl {
       \int_a^b f(x) \sin (\omega x)~dx
       \f]
       is computed for some frequency parameter \f$ \omega \f$,
-      stored in \ref inte_qawo_gsl_sin::omega .
+      stored in \ref o2scl::inte_qawo_gsl_sin::omega .
       
       An adaptive algorithm together with an series-acceleration
-      method like that of \ref inte_qags_gsl is used. Those
+      method like that of \ref o2scl::inte_qags_gsl is used. Those
       subintervals with "large" widths \f$ d \equiv b-a \f$ where \f$
       d\omega > 4 \f$ are computed using a 25-point Clenshaw-Curtis
       integration rule to handle the oscillatory behavior. In order to
@@ -639,7 +639,7 @@ namespace o2scl {
       \f]
       is computed for some frequency parameter \f$ \omega \f$ .
 
-      This class is exactly analogous to \ref inte_qawo_gsl_sin .
+      This class is exactly analogous to \ref o2scl::inte_qawo_gsl_sin .
       See that class documentation for more details.
   */
   template<class func_t> class inte_qawo_gsl_cos : 

src/inte/inte_singular_gsl.h

@@ -55,7 +55,7 @@ namespace o2scl {
 
   public:
 
-    /** \brief A structure for extrapolation for \ref inte_qags_gsl
+    /** \brief A structure for extrapolation for \ref o2scl::inte_qags_gsl
 
 	\future Move this to a new class, with qelg() as a method
     */

src/part/fermion_nonrel.h

@@ -289,13 +289,18 @@ namespace o2scl {
     return 0;
   }
 
-
+  /** \brief Compute thermodynamics with antiparticles at fixed
+      chemical potential (unimplemented)
+   */
   virtual void pair_mu(fermion &f, fp_t temper) {
     O2SCL_ERR2("Function fermion_nonrel::pair_mu() not ",
 	       "implemented.",exc_eunimpl);
     return;
   }
 
+  /** \brief Compute thermodynamics with antiparticles at fixed
+      density (unimplemented)
+   */
   virtual int pair_density(fermion &f, fp_t temper) {
     O2SCL_ERR2("Function fermion_nonrel::pair_density() not ",
 	       "implemented.",exc_eunimpl);