Chosen Fixed Point
Here is the data for the chosen fixed point.
$F_{UV}$ represents the flavor symmetries in the UV Lagrangian, and $F_{IR}$ represents the flavor symmetries in the IR. $F_{UV}$ and $F_{IR}$ can differ due to accidental symmetry enhancement.
The number of marginal operators, $n_{marginal}$, minus the dimension of flavor symmetries in IR, $|F_{IR}|$, corresponds to the coefficient of $t^6$ in the superconformal index.
| # | Theory | Superpotential | Central charge $a$ | Central charge $c$ | Ratio $a/c$ | Matter field: $R$-charge | U(1) part of $F_{UV}$ | Rank of $F_{UV}$ | Rational |
|---|---|---|---|---|---|---|---|---|---|
| 60070 | SU3adj1nf2 | ${}M_{1}\phi_{1}q_{1}\tilde{q}_{1}$ + ${ }M_{1}q_{2}\tilde{q}_{1}$ + ${ }\phi_{1}^{2}X_{1}$ + ${ }\phi_{1}\tilde{q}_{1}^{2}\tilde{q}_{2}$ + ${ }q_{1}^{2}\tilde{q}_{2}^{2}$ | 1.3914 | 1.5625 | 0.8905 | [X:[1.4204], M:[0.7388], q:[0.4109, 0.7007], qb:[0.5605, 0.5891], phi:[0.2898]] | [X:[[6]], M:[[-18]], q:[[13], [10]], qb:[[8], [-13]], phi:[[-3]]] | 1 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| ${}M_{1}$, ${ }\phi_{1}^{3}$, ${ }q_{1}\tilde{q}_{1}$, ${ }q_{1}\tilde{q}_{2}$, ${ }q_{2}\tilde{q}_{1}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }q_{2}\tilde{q}_{2}$, ${ }X_{1}$, ${ }M_{1}^{2}$, ${ }\phi_{1}^{2}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}^{2}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }M_{1}\phi_{1}^{3}$, ${ }\phi_{1}^{6}$, ${ }M_{1}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{1}^{2}q_{2}$, ${ }\phi_{1}^{3}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}^{3}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{2}$, ${ }q_{1}^{2}\tilde{q}_{1}^{2}$ | ${}$ | -2 | t^2.22 + t^2.61 + t^2.91 + t^3. + t^3.78 + 2*t^3.87 + t^4.26 + t^4.43 + 2*t^4.65 + 2*t^4.74 + t^4.82 + 2*t^5.22 + t^5.44 + 2*t^5.52 + 2*t^5.61 + t^5.83 - 2*t^6. + 2*t^6.09 + 3*t^6.31 + t^6.39 + 3*t^6.48 + t^6.65 + t^6.7 + 2*t^6.78 + t^6.87 + 2*t^6.96 + t^7.04 + 3*t^7.18 + 3*t^7.26 + t^7.35 + 2*t^7.43 + t^7.57 + 5*t^7.65 + 4*t^7.74 + 3*t^7.82 + t^7.91 + 2*t^8.04 + 2*t^8.13 - 2*t^8.22 + t^8.3 + t^8.35 + 2*t^8.44 + 8*t^8.52 + 3*t^8.61 + 3*t^8.69 + t^8.74 + t^8.87 + t^8.61/y^2 - t^3.87/y - t^4.74/y - t^6.09/y - t^6.48/y - t^6.78/y - t^6.87/y - t^6.96/y - t^7.35/y - t^7.65/y - (2*t^7.74)/y + t^7.82/y + t^8.13/y + t^8.22/y - t^8.3/y - t^8.61/y - t^8.69/y + t^8.91/y - t^3.87*y - t^4.74*y - t^6.09*y - t^6.48*y - t^6.78*y - t^6.87*y - t^6.96*y - t^7.35*y - t^7.65*y - 2*t^7.74*y + t^7.82*y + t^8.13*y + t^8.22*y - t^8.3*y - t^8.61*y - t^8.69*y + t^8.91*y + t^8.61*y^2 | t^2.22/g1^18 + t^2.61/g1^9 + g1^21*t^2.91 + t^3. + g1^18*t^3.78 + (2*t^3.87)/g1^3 + g1^6*t^4.26 + t^4.43/g1^36 + 2*g1^15*t^4.65 + (2*t^4.74)/g1^6 + t^4.82/g1^27 + (2*t^5.22)/g1^18 + g1^33*t^5.44 + 2*g1^12*t^5.52 + (2*t^5.61)/g1^9 + g1^42*t^5.83 - 2*t^6. + (2*t^6.09)/g1^21 + 3*g1^30*t^6.31 + g1^9*t^6.39 + (3*t^6.48)/g1^12 + t^6.65/g1^54 + g1^39*t^6.7 + 2*g1^18*t^6.78 + t^6.87/g1^3 + (2*t^6.96)/g1^24 + t^7.04/g1^45 + 3*g1^27*t^7.18 + 3*g1^6*t^7.26 + t^7.35/g1^15 + (2*t^7.43)/g1^36 + g1^36*t^7.57 + 5*g1^15*t^7.65 + (4*t^7.74)/g1^6 + (3*t^7.82)/g1^27 + t^7.91/g1^48 + 2*g1^24*t^8.04 + 2*g1^3*t^8.13 - (2*t^8.22)/g1^18 + t^8.3/g1^39 + g1^54*t^8.35 + 2*g1^33*t^8.44 + 8*g1^12*t^8.52 + (3*t^8.61)/g1^9 + (3*t^8.69)/g1^30 + g1^63*t^8.74 + t^8.87/g1^72 + t^8.61/(g1^9*y^2) - t^3.87/(g1^3*y) - t^4.74/(g1^6*y) - t^6.09/(g1^21*y) - t^6.48/(g1^12*y) - (g1^18*t^6.78)/y - t^6.87/(g1^3*y) - t^6.96/(g1^24*y) - t^7.35/(g1^15*y) - (g1^15*t^7.65)/y - (2*t^7.74)/(g1^6*y) + t^7.82/(g1^27*y) + (g1^3*t^8.13)/y + t^8.22/(g1^18*y) - t^8.3/(g1^39*y) - t^8.61/(g1^9*y) - t^8.69/(g1^30*y) + (g1^21*t^8.91)/y - (t^3.87*y)/g1^3 - (t^4.74*y)/g1^6 - (t^6.09*y)/g1^21 - (t^6.48*y)/g1^12 - g1^18*t^6.78*y - (t^6.87*y)/g1^3 - (t^6.96*y)/g1^24 - (t^7.35*y)/g1^15 - g1^15*t^7.65*y - (2*t^7.74*y)/g1^6 + (t^7.82*y)/g1^27 + g1^3*t^8.13*y + (t^8.22*y)/g1^18 - (t^8.3*y)/g1^39 - (t^8.61*y)/g1^9 - (t^8.69*y)/g1^30 + g1^21*t^8.91*y + (t^8.61*y^2)/g1^9 |
Deformation
Here is the data for the deformed fixed points from the chosen fixed point.
| # | Superpotential | Central Charge $a$ | Central Charge $c$ | Ratio $a/c$ | $R$-charges | Superconformal Index | More Info. | Rational |
|---|
Equivalent Fixed Points from Other Seed Theories
Here is a list of equivalent fixed points from other gauge theories.
| # | Theory | Superpotential | Central Charge $a$ | Central Charge $c$ | Ratio $a/c$ | $R$-charges | Superconformal Index | More Info. | Rational |
|---|
Equivalent Fixed Points from the Same Seed Theory
Below is a list of equivalent fixed points from the same seed theories.
| id | Theory | Superpotential | Central Charge $a$ | Central Charge $c$ | Ratio $a/c$ | $R$-charges | More Info. | Rational |
|---|
Previous Theory
The previous fixed point before deforming to get the chosen fixed point.
| # | Theory | Superpotential | Central Charge $a$ | Central Charge $c$ | Ratio $a/c$ | $R$-charges | Superconformal Index | More Info. | Rational |
|---|---|---|---|---|---|---|---|---|---|
| 57494 | SU3adj1nf2 | ${}M_{1}\phi_{1}q_{1}\tilde{q}_{1}$ + ${ }M_{1}q_{2}\tilde{q}_{1}$ + ${ }\phi_{1}^{2}X_{1}$ + ${ }\phi_{1}\tilde{q}_{1}^{2}\tilde{q}_{2}$ | 1.3992 | 1.5824 | 0.8843 | [X:[1.3887], M:[0.7377], q:[0.3742, 0.6799], qb:[0.5824, 0.5296], phi:[0.3057]] | t^2.21 + t^2.71 + t^2.75 + t^2.87 + 2*t^3.63 + t^3.79 + t^4.17 + t^4.43 + 2*t^4.55 + 2*t^4.7 + t^4.92 + t^4.96 + t^5.2 + t^5.42 + 2*t^5.46 + t^5.5 + t^5.58 + 2*t^5.62 + t^5.74 + 2*t^5.84 - 3*t^6. - t^3.92/y - t^4.83/y - t^3.92*y - t^4.83*y | detail |