These results, and their nondimensionalization, are described in D.J. Lusher & G.N. Coleman (LC23):
"Numerical study of compressible wall-bounded turbulence -- the effect of thermal wall boundary conditions 
on the turbulent Prandtl number in the low-supersonic regime",
International J. Computational Fluid Dynamics, 2023 (https://doi.org/10.1080/10618562.2023.2189247)

Files are in Tecplot ascii( .dat ) format, and named by Case (see Table 1 of LC23).

The following quantities are included:

 Y  
 mean_ww           (< w w >)
 mean_rhow         (< \rho w >)
 mean_rhovw        (< \rho v w >)
 mean_TT           (< T T >)
 mean_rhouv        (< \rho u v >)
 mean_E            (< E >)
 mean_uv           (< u v >)
 mean_vv           (< v v >)
 mean_rhouw        (< \rho u w >)
 mean_rhorho       (< \rho \rho >)
 mean_rhou         (< \rho u >)
 mean_rhov         (< \rho v >)
 mean_pp           (< p p >)
 mean_rhoww        (< \rho w w >)
 mean_W            (< w >)
 mean_rhoTv        (< \rho T v >)
 mean_M            (< M >)
 mean_uw           (< u w >)
 mean_p            (< p >)
 mean_a            (< a >)
 mean_T            (< T >)
 mean_rhouu        (< \rho u u >)
 mean_rho          (< \rho >)
 mean_mu           (< \mu >)
 mean_vw           (< v w >)
 mean_uu           (< u u >)
 mean_rhovv        (< \rho v v >)
 mean_U            (< u >)
 mean_V            (< v >)
 mean_dilatsq      (< u_{i,i} u_{j,j} >)
 mean_vortsq       (< \omega_i \omega_i >)
 mean_rhoTdilat    (< \rho T \w u_{i,i} >)
 mean_duidxjtauij  (< u_{i,j} \tau_{ij} >)
 mean_mudTdy       (< \mu T_{,2} >)
 mean_mududy       (< \mu u_{1,2} >)
 mean_Tv           (< T v >)
 mean_pu           (< p u >)
 mean_mudotu       (< \mu u >)
 mean_mudotv       (< \mu v >)
 mean_mudotw       (< \mu w >)
 mean_muT          (< \mu T >)
 mean_rhoTT        (< \rho T T >)
 mean_rhovuu       (< \rho v u u >)
 mean_rhovvv       (< \rho v v v >)
 mean_rhovww       (< \rho v w w >)
 mean_rhouvv       (< \rho u v v >)
 mean_pdudx        (< p u_{1,1} >)
 mean_pdvdy        (< p u_{2,2} >)
 mean_pdwdz        (< p u_{3,3} >)
 mean_pdudy        (< p u_{1,2} >)
 mean_pdvdx        (< p u_{2,1} >)
 mean_muduudy      (< \mu {uu}_{,2} >)
 mean_mudvvdy      (< \mu {vv}_{,2} >)
 mean_mudwwdy      (< \mu {ww}_{,2} >)
 mean_muduvdy      (< \mu {uv}_{,2} >)
 mean_tau12        (< \tau_{12} >)
 mean_utau12       (< u \tau_{12} >)
 mean_tau22        (< \tau_{22} >)
 mean_vtau22       (< v \tau{22} >)
 mean_tau23        (< \tau_{23} >)
 mean_wtau23       (< w \tau_{23} >)

Notes:
1. Variable definitions and normalization scheme are given in LC23.
2. The prefix "mean"  denotes a Reynolds average (indicated in LC23 by angle brackets "<.>").
3. All of the above statistics have been formed in terms of their total (i.e. "pre-Reynolds/Favre-decomposed") form; for example, u_i = <u_i> + u'_i, \omega_i = <\omega_i> + \omega'_i, T = <T> + T', etc.
4. Files for Cases iiA and aiB contain only a partial set of the above quantitities.  If the full set for Case aiB (and a    few alternative statistics for Case iiA) is desired, contact GNC at email address below.

Update (2025/12): Two new higher Reynolds number versions of cases: aiE2s and aiF2 have been added to the DNS database as follows:

(Re_\tau - isothermal/adiabatic sides)

aiE2s (IJCFD, 2023) - (1200/2400)
aiE2s_2025 - (1250/3937.5)

aiF2 (IJCFD, 2023) - (1070/2354)
aiF2_2025 (1575/3937.5)

Please direct queries to g.n.coleman@nasa.gov or lusher.david@jaxa.jp