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Getting masses and weak-scale parameters

Look at the output (S1.msugra). It should begin like this:

 ********************************************
 *                                          *
 *  ISAJET     V7.58   22-AUG-2001 14:30:33 *
 *                                          *
 ********************************************



 Minimal supergravity (mSUGRA) model:

 M_0,  M_(1/2),  A_0,  tan(beta),  sgn(mu),  M_t =
   100.000   250.000     0.000    10.000     1.0   175.000

 ISASUGRA unification:
 M_GUT      = 0.218E+17   g_GUT          =0.714      alpha_GUT =0.041
 FT_GUT     = 0.482       FB_GUT         = 0.047     FL_GUT = 0.069

 1/alpha_em =  127.71     sin**2(thetaw) =0.2310     alpha_s   =0.119
 M_1        =   99.04     M_2            =  192.49   M_3       =  580.19
 mu(Q)      =  333.22     B(Q)           =   43.23   Q         =  459.88
 M_H1^2     = 0.339E+05   M_H2^2         =-0.110E+06

 ISAJET masses (with signs):
 M(GL)  =   595.07
 M(UL)  =   537.00   M(UR)  =   520.23   M(DL)  =   542.80   M(DR) =   519.91
 M(B1)  =   495.22   M(B2)  =   524.66   M(T1)  =   393.57   M(T2) =   573.59
 M(SN)  =   185.93   M(EL)  =   202.08   M(ER)  =   142.92
 M(NTAU)=   185.23   M(TAU1)=   134.84   M(TAU2)=   205.65
 M(Z1)  =   -95.62   M(Z2)  =  -174.73   M(Z3)  =   339.90   M(Z4) =  -361.08
 M(W1)  =  -174.14   M(W2)  =  -361.39
 M(HL)  =   113.04   M(HH)  =   377.80   M(HA)  =   377.23   M(H+) =   385.71

 theta_t=   0.9628   theta_b=   0.5189   theta_l=   1.3041   alpha_h=   0.1121

 NEUTRALINO MASSES (SIGNED) =   -95.616  -174.729   339.898  -361.078
 EIGENVECTOR 1       =   0.06075  -0.16150  -0.06315   0.98298
 EIGENVECTOR 2       =   0.17761  -0.29938  -0.92976  -0.11990
 EIGENVECTOR 3       =  -0.71086  -0.69383   0.09586  -0.06390
 EIGENVECTOR 4       =   0.67782  -0.63473   0.34981  -0.12370

 CHARGINO MASSES (SIGNED)  =  -174.141  -361.392
 GAMMAL, GAMMAR             =   2.02660   1.83631


 ISAJET equivalent input:
 MSSMA:   595.07  333.22  377.23   10.00
 MSSMB:   539.62  519.30  521.44  196.58  136.18
 MSSMC:   499.18  516.95  432.66  195.92  134.20 -474.93 -689.38 -157.35
 MSSMD: SAME AS MSSMB (DEFAULT)
 MSSME:    99.04  192.49
 WARNING IN SSXINT: BAD CONVERGENCE FOR           74 INTERVALS.

The first line of data repeats the input (although slightly misjustified). A little further down (where it says ISAJET masses (with signs)), you can find the masses of the particles. These are mostly quite intuitive, but can be checked against older documents on the parameter points if needed.

The weak-scale parameters are found mostly in the lines that begin MSSMX at the bottom of the section shown above. More specifically, the paramters can be found as follows:

$\mu$ 333.22 Second listing after MSSMA:
$m_{\tilde{g}}$ 595.07 First listing after MSSMA:
$m_{A^0}$ 377.23 Third listing after MSSMA:
$m_{\tilde{q}_1}$ 539.62 First listing after MSSMB:
$m_{\tilde{d}_R}$ 519.30 Second listing after MSSMB:
$m_{\tilde{u}_R}$ 521.44 Third listing after MSSMB:
$m_{\tilde{\ell}_1}$ 196.58 Fourth listing after MSSMB:
$m_{\tilde{e}_r}$ 136.18 Fifth listing after MSSMB:
$m_{\tilde{q}_3}$ 499.18 First listing after MSSMC:
$m_{\tilde{b}_r}$ 516.95 Second listing after MSSMC:
$m_{\tilde{t}_r}$ 432.66 Third listing after MSSMC:
$m_{\tilde{\ell}_3}$ 195.92 Fourth listing after MSSMC:
$m_{\tilde{\tau}_r}$ 134.20 Fifth listing after MSSMC:
$A_t$ -474.93 Third-to-last number after MSSMC:
$A_b$ -689.38 Second-to-last number after MSSMC:
$A_\tau$ -157.35 Last number after MSSMC:

The sparticle masses are much more straightforward. These are listed under ISAJET masses with signs. The masses are as follows:

\ensuremath{\widetilde{g}} M(GL)            
$\ensuremath{\widetilde{u}}_L$ M(UL) $\ensuremath{\widetilde{u}}_R$ M(UR) $\ensuremath{\widetilde{d}}_L$ M(DL) $\ensuremath{\widetilde{d}}_R$ M(DR)
$\ensuremath{\widetilde{b}}_1$ M(B1) $\ensuremath{\widetilde{b}}_2$ M(B2) $\ensuremath{\widetilde{t}}_1$ M(T1) $\ensuremath{\widetilde{t}}_2$ M(T2)
\ensuremath{\widetilde{\nu}_\ell} M(SN) \ensuremath{\widetilde{e}_L^\pm} M(EL) \ensuremath{\widetilde{e}_R^\pm} M(ER)    
\ensuremath{\widetilde{\nu}_\tau} M(NTAU) \ensuremath{\widetilde{\tau}_1^\pm} M(TAU1) \ensuremath{\widetilde{\tau}_2^\pm} M(TAU2)    
\ensuremath{\widetilde{\chi}_1^0} M(Z1) \ensuremath{\widetilde{\chi}_2^0} M(Z2) \ensuremath{\widetilde{\chi}_3^0} M(Z3) \ensuremath{\widetilde{\chi}_4^0} M(Z4)
$\ensuremath{\widetilde{\chi}_1^\pm}$ M(W1) \ensuremath{\widetilde{\chi}_2^\pm} M(W2)        
$h^0$ M(HL) $H^0$ M(HH) $A^0$ M(HA) $H^+$ M(H+)


next up previous
Next: Running ISASUSY Up: Generating SUSY Cross Sections Previous: Runnin ISASUGRA
Joseph William Proulx 2001-10-26