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 |
|---|---|---|---|---|---|---|---|---|---|
| 3590 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{3}q_{1}\tilde{q}_{1}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{5}q_{2}\tilde{q}_{1}$ + ${ }M_{4}M_{5}$ + ${ }M_{2}M_{3}$ + ${ }\phi_{1}q_{1}q_{2}$ + ${ }M_{1}X_{1}$ + ${ }M_{6}\phi_{1}\tilde{q}_{2}^{2}$ + ${ }M_{4}M_{7}$ | 0.577 | 0.7207 | 0.8006 | [X:[1.575], M:[0.425, 1.2751, 0.7249, 0.9752, 1.0248, 0.8004, 1.0248], q:[0.9374, 0.6375], qb:[0.3376, 0.3873], phi:[0.425]] | [X:[[2]], M:[[-2], [-6], [6], [-14], [14], [-32], [14]], q:[[5], [-3]], qb:[[-11], [17]], phi:[[-2]]] | 1 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| ${}M_{3}$, ${ }M_{6}$, ${ }\phi_{1}^{2}$, ${ }M_{5}$, ${ }M_{7}$, ${ }\phi_{1}\tilde{q}_{1}^{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{2}$, ${ }q_{1}\tilde{q}_{2}$, ${ }M_{3}^{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }M_{3}M_{6}$, ${ }M_{3}\phi_{1}^{2}$, ${ }X_{1}$, ${ }M_{6}^{2}$, ${ }M_{6}\phi_{1}^{2}$, ${ }\phi_{1}^{4}$, ${ }\phi_{1}q_{2}^{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }M_{3}M_{5}$, ${ }M_{3}M_{7}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }M_{5}M_{6}$, ${ }M_{6}M_{7}$, ${ }M_{3}\phi_{1}\tilde{q}_{1}^{2}$, ${ }M_{5}\phi_{1}^{2}$, ${ }M_{7}\phi_{1}^{2}$, ${ }M_{3}\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{6}\phi_{1}\tilde{q}_{1}^{2}$, ${ }\phi_{1}^{3}\tilde{q}_{1}^{2}$, ${ }M_{6}\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$ | ${}\phi_{1}^{3}\tilde{q}_{1}\tilde{q}_{2}$ | -1 | t^2.175 + t^2.401 + t^2.55 + 2*t^3.075 + t^3.301 + t^3.45 + t^3.825 + t^3.974 + t^4.35 + t^4.576 + 2*t^4.725 + t^4.802 + t^4.951 + t^5.1 + 2*t^5.249 + 2*t^5.476 + 2*t^5.625 + t^5.702 + t^5.851 - t^6. + 3*t^6.149 + t^6.226 + 2*t^6.375 + 2*t^6.524 + t^6.602 + t^6.9 + t^6.977 + t^7.049 + 2*t^7.126 + t^7.203 + t^7.275 + t^7.352 + t^7.424 + t^7.501 + 2*t^7.65 + 3*t^7.799 + 2*t^7.877 + t^7.949 + t^8.026 + t^8.103 - t^8.175 + t^8.252 + 2*t^8.324 - t^8.401 + t^8.55 + t^8.627 + 2*t^8.699 + 2*t^8.776 - t^4.275/y - t^6.676/y - t^6.825/y + t^7.201/y - t^7.35/y + t^7.576/y + (2*t^7.725)/y + t^7.874/y + t^7.951/y + (2*t^8.249)/y + (3*t^8.476)/y + (3*t^8.625)/y + t^8.702/y + (2*t^8.851)/y - t^4.275*y - t^6.676*y - t^6.825*y + t^7.201*y - t^7.35*y + t^7.576*y + 2*t^7.725*y + t^7.874*y + t^7.951*y + 2*t^8.249*y + 3*t^8.476*y + 3*t^8.625*y + t^8.702*y + 2*t^8.851*y | g1^6*t^2.175 + t^2.401/g1^32 + t^2.55/g1^4 + 2*g1^14*t^3.075 + t^3.301/g1^24 + g1^4*t^3.45 + t^3.825/g1^6 + g1^22*t^3.974 + g1^12*t^4.35 + t^4.576/g1^26 + 2*g1^2*t^4.725 + t^4.802/g1^64 + t^4.951/g1^36 + t^5.1/g1^8 + 2*g1^20*t^5.249 + (2*t^5.476)/g1^18 + 2*g1^10*t^5.625 + t^5.702/g1^56 + t^5.851/g1^28 - t^6. + 3*g1^28*t^6.149 + t^6.226/g1^38 + (2*t^6.375)/g1^10 + 2*g1^18*t^6.524 + t^6.602/g1^48 + g1^8*t^6.9 + t^6.977/g1^58 + g1^36*t^7.049 + (2*t^7.126)/g1^30 + t^7.203/g1^96 + t^7.275/g1^2 + t^7.352/g1^68 + g1^26*t^7.424 + t^7.501/g1^40 + (2*t^7.65)/g1^12 + 3*g1^16*t^7.799 + (2*t^7.877)/g1^50 + g1^44*t^7.949 + t^8.026/g1^22 + t^8.103/g1^88 - g1^6*t^8.175 + t^8.252/g1^60 + 2*g1^34*t^8.324 - t^8.401/g1^32 + t^8.55/g1^4 + t^8.627/g1^70 + 2*g1^24*t^8.699 + (2*t^8.776)/g1^42 - t^4.275/(g1^2*y) - t^6.676/(g1^34*y) - t^6.825/(g1^6*y) + t^7.201/(g1^16*y) - (g1^12*t^7.35)/y + t^7.576/(g1^26*y) + (2*g1^2*t^7.725)/y + (g1^30*t^7.874)/y + t^7.951/(g1^36*y) + (2*g1^20*t^8.249)/y + (3*t^8.476)/(g1^18*y) + (3*g1^10*t^8.625)/y + t^8.702/(g1^56*y) + (2*t^8.851)/(g1^28*y) - (t^4.275*y)/g1^2 - (t^6.676*y)/g1^34 - (t^6.825*y)/g1^6 + (t^7.201*y)/g1^16 - g1^12*t^7.35*y + (t^7.576*y)/g1^26 + 2*g1^2*t^7.725*y + g1^30*t^7.874*y + (t^7.951*y)/g1^36 + 2*g1^20*t^8.249*y + (3*t^8.476*y)/g1^18 + 3*g1^10*t^8.625*y + (t^8.702*y)/g1^56 + (2*t^8.851*y)/g1^28 |
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 |
|---|---|---|---|---|---|---|---|---|---|
| 2982 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{3}q_{1}\tilde{q}_{1}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{5}q_{2}\tilde{q}_{1}$ + ${ }M_{4}M_{5}$ + ${ }M_{2}M_{3}$ + ${ }\phi_{1}q_{1}q_{2}$ + ${ }M_{1}X_{1}$ + ${ }M_{6}\phi_{1}\tilde{q}_{2}^{2}$ | 0.58 | 0.7267 | 0.7981 | [X:[1.577], M:[0.423, 1.2689, 0.7311, 0.9607, 1.0393, 0.7673], q:[0.9426, 0.6344], qb:[0.3263, 0.4049], phi:[0.423]] | t^2.193 + t^2.302 + t^2.538 + t^2.882 + t^3.118 + t^3.226 + t^3.462 + t^3.807 + t^4.042 + t^4.387 + t^4.495 + t^4.604 + 2*t^4.731 + t^4.84 + 2*t^5.075 + t^5.184 + t^5.311 + 2*t^5.42 + t^5.528 + t^5.656 + 2*t^5.764 - t^4.269/y - t^4.269*y | detail |