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 |
|---|---|---|---|---|---|---|---|---|---|
| 61202 | SU3adj1nf2 | ${}\phi_{1}q_{1}^{2}q_{2}$ + ${ }\phi_{1}^{2}X_{1}$ + ${ }M_{1}\phi_{1}q_{2}\tilde{q}_{1}$ + ${ }M_{1}q_{1}\tilde{q}_{1}$ + ${ }M_{2}q_{2}\tilde{q}_{1}$ + ${ }M_{3}q_{2}\tilde{q}_{2}$ | 1.3829 | 1.5563 | 0.8886 | [X:[1.3883], M:[0.7543, 1.0601, 1.0808], q:[0.6667, 0.3608], qb:[0.5791, 0.5583], phi:[0.3059]] | [X:[[0, 2]], M:[[1, -5], [1, -6], [-1, -1]], q:[[0, 0], [0, 1]], qb:[[-1, 5], [1, 0]], phi:[[0, -1]]] | 2 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| ${}M_{1}$, ${ }\phi_{1}^{3}$, ${ }M_{2}$, ${ }M_{3}$, ${ }q_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }q_{1}\tilde{q}_{1}$, ${ }X_{1}$, ${ }M_{1}^{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{1}$, ${ }M_{1}\phi_{1}^{3}$, ${ }M_{1}M_{2}$, ${ }M_{1}M_{3}$, ${ }\phi_{1}^{6}$, ${ }\phi_{1}^{2}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}^{2}q_{1}\tilde{q}_{1}$, ${ }M_{2}\phi_{1}^{3}$, ${ }M_{1}q_{1}\tilde{q}_{2}$ | ${}M_{3}\phi_{1}^{3}$, ${ }\phi_{1}^{3}q_{2}^{3}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}^{2}$ | 1 | t^2.26 + t^2.75 + t^3.18 + t^3.24 + 2*t^3.68 + t^3.74 + t^4.16 + t^4.53 + 2*t^4.59 + 2*t^4.65 + t^5.02 + t^5.44 + 3*t^5.51 + t^5.57 + t^5.93 + t^5.94 + t^6. - t^6.06 + t^6.07 + t^6.36 + t^6.42 + 3*t^6.43 + 2*t^6.49 + t^6.79 + 3*t^6.86 + 4*t^6.92 + t^6.98 + t^7.28 + 4*t^7.35 + 2*t^7.41 + t^7.47 + t^7.71 + 4*t^7.77 + t^7.78 + 5*t^7.84 + 2*t^7.9 + t^7.96 + 2*t^8.2 + 4*t^8.27 - 2*t^8.32 + 4*t^8.33 + t^8.39 + t^8.62 + 5*t^8.69 + 4*t^8.75 + t^8.76 + t^8.82 + t^8.75/y^2 - t^3.92/y - t^4.84/y - t^6.18/y - t^6.67/y - (2*t^7.1)/y - t^7.16/y - (2*t^7.59)/y - t^8.08/y - t^8.51/y - t^8.57/y + (2*t^8.94)/y - t^3.92*y - t^4.84*y - t^6.18*y - t^6.67*y - 2*t^7.1*y - t^7.16*y - 2*t^7.59*y - t^8.08*y - t^8.51*y - t^8.57*y + 2*t^8.94*y + t^8.75*y^2 | (g1*t^2.26)/g2^5 + t^2.75/g2^3 + (g1*t^3.18)/g2^6 + t^3.24/(g1*g2) + 2*g1*t^3.68 + (g2^5*t^3.74)/g1 + g2^2*t^4.16 + (g1^2*t^4.53)/g2^10 + (2*g1*t^4.59)/g2 + (2*g2^4*t^4.65)/g1 + (g1*t^5.02)/g2^8 + (g1^2*t^5.44)/g2^11 + (2*t^5.51)/g2^6 + (g1*t^5.51)/g2^2 + (g2^3*t^5.57)/g1 + (g1*t^5.93)/g2^9 + (g1^2*t^5.94)/g2^5 - t^6. + t^6./(g1*g2^4) + g1*g2^4*t^6. - (g2^5*t^6.06)/g1^2 + (g2^9*t^6.07)/g1 + (g1^2*t^6.36)/g2^12 + t^6.42/g2^7 + (3*g1*t^6.43)/g2^3 + t^6.49/(g1^2*g2^2) + (g2^2*t^6.49)/g1 + (g1^3*t^6.79)/g2^15 + (3*g1^2*t^6.86)/g2^6 + (3*t^6.92)/g2 + g1*g2^3*t^6.92 + (g2^8*t^6.98)/g1 + (g1^2*t^7.28)/g2^13 + 3*g1^2*t^7.35 + (g1*t^7.35)/g2^4 + (g2*t^7.41)/g1 + g2^5*t^7.41 + (g2^10*t^7.47)/g1^2 + (g1^3*t^7.71)/g2^16 + (2*g1*t^7.77)/g2^11 + (2*g1^2*t^7.77)/g2^7 + (g1^3*t^7.78)/g2^3 + (3*t^7.84)/g2^2 + 2*g1*g2^2*t^7.84 + (g2^3*t^7.9)/g1^2 + (g2^7*t^7.9)/g1 + (g2^12*t^7.96)/g1^3 + (g1^2*t^8.2)/g2^14 + (g1^3*t^8.2)/g2^10 + (2*t^8.26)/g2^9 - (2*g1*t^8.26)/g2^5 + (4*g1^2*t^8.27)/g2 - (2*t^8.32)/g1 + 4*g2^4*t^8.33 + (g2^9*t^8.39)/g1^2 + (g1^3*t^8.62)/g2^17 + (2*g1*t^8.69)/g2^12 + (3*g1^2*t^8.69)/g2^8 + (2*t^8.75)/(g1*g2^7) + (2*t^8.75)/g2^3 + g1*g2*t^8.76 + (g2^6*t^8.82)/g1 + t^8.75/(g2^3*y^2) - t^3.92/(g2*y) - t^4.84/(g2^2*y) - (g1*t^6.18)/(g2^6*y) - t^6.67/(g2^4*y) - (2*g1*t^7.1)/(g2^7*y) - t^7.16/(g1*g2^2*y) - t^7.59/(g2^5*y) - (g1*t^7.59)/(g2*y) - t^8.08/(g1*g2^3*y) + t^8.51/(g2^6*y) - (2*g1*t^8.51)/(g2^2*y) - (g2^3*t^8.57)/(g1*y) + (2*g1^2*t^8.94)/(g2^5*y) - (t^3.92*y)/g2 - (t^4.84*y)/g2^2 - (g1*t^6.18*y)/g2^6 - (t^6.67*y)/g2^4 - (2*g1*t^7.1*y)/g2^7 - (t^7.16*y)/(g1*g2^2) - (t^7.59*y)/g2^5 - (g1*t^7.59*y)/g2 - (t^8.08*y)/(g1*g2^3) + (t^8.51*y)/g2^6 - (2*g1*t^8.51*y)/g2^2 - (g2^3*t^8.57*y)/g1 + (2*g1^2*t^8.94*y)/g2^5 + (t^8.75*y^2)/g2^3 |
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 |
|---|---|---|---|---|---|---|---|---|---|
| 58612 | SU3adj1nf2 | ${}\phi_{1}q_{1}^{2}q_{2}$ + ${ }\phi_{1}^{2}X_{1}$ + ${ }M_{1}\phi_{1}q_{2}\tilde{q}_{1}$ + ${ }M_{1}q_{1}\tilde{q}_{1}$ + ${ }M_{2}q_{2}\tilde{q}_{1}$ | 1.3924 | 1.5762 | 0.8834 | [X:[1.3724], M:[0.7554, 1.0692], q:[0.6667, 0.3529], qb:[0.5779, 0.5197], phi:[0.3138]] | t^2.27 + t^2.62 + t^2.82 + t^3.21 + 2*t^3.56 + t^3.73 + t^4.12 + 2*t^4.5 + t^4.53 + 2*t^4.68 + t^4.88 + t^5.09 + t^5.24 + 2*t^5.44 + t^5.47 + t^5.62 + t^5.65 + t^5.79 + 2*t^5.83 + t^5.97 - t^6. - t^3.94/y - t^4.88/y - t^3.94*y - t^4.88*y | detail |