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 |
|---|---|---|---|---|---|---|---|---|---|
| 57522 | SU2adj1nf2 | ${}M_{1}\phi_{1}^{2}$ + ${ }M_{2}q_{1}q_{2}$ + ${ }M_{3}q_{1}\tilde{q}_{1}$ + ${ }M_{4}q_{2}\tilde{q}_{1}$ + ${ }\phi_{1}\tilde{q}_{2}^{2}$ + ${ }M_{2}M_{4}$ + ${ }M_{5}q_{1}\tilde{q}_{2}$ + ${ }M_{3}M_{5}$ + ${ }M_{3}M_{6}$ + ${ }M_{7}\phi_{1}q_{1}\tilde{q}_{1}$ | 0.6715 | 0.835 | 0.8043 | [M:[1.0962, 1.0291, 1.1633, 0.9709, 0.8367, 0.8367, 0.7114], q:[0.3892, 0.5816], qb:[0.4475, 0.7741], phi:[0.4519]] | [M:[[4], [22], [-14], [-22], [14], [14], [-12]], q:[[-15], [-7]], qb:[[29], [1]], phi:[[-2]]] | 1 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| ${}M_{7}$, ${ }M_{5}$, ${ }M_{6}$, ${ }M_{4}$, ${ }M_{2}$, ${ }M_{1}$, ${ }\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{1}^{2}$, ${ }\phi_{1}\tilde{q}_{1}^{2}$, ${ }q_{2}\tilde{q}_{2}$, ${ }M_{7}^{2}$, ${ }\phi_{1}q_{1}q_{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }M_{5}M_{7}$, ${ }M_{6}M_{7}$, ${ }\phi_{1}q_{2}^{2}$, ${ }M_{5}^{2}$, ${ }M_{5}M_{6}$, ${ }M_{6}^{2}$, ${ }M_{4}M_{7}$, ${ }M_{2}M_{7}$, ${ }M_{4}M_{5}$, ${ }M_{4}M_{6}$, ${ }M_{1}M_{7}$, ${ }M_{2}M_{5}$, ${ }M_{2}M_{6}$, ${ }M_{1}M_{5}$, ${ }M_{1}M_{6}$, ${ }M_{7}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{4}^{2}$, ${ }M_{7}\phi_{1}q_{1}^{2}$ | ${}$ | -2 | t^2.134 + 2*t^2.51 + t^2.913 + t^3.087 + t^3.289 + t^3.665 + t^3.691 + t^4.04 + t^4.067 + 2*t^4.268 + t^4.443 + 2*t^4.644 + t^4.846 + 3*t^5.02 + t^5.047 + t^5.222 + 2*t^5.423 + t^5.597 + 3*t^5.799 + t^5.825 - 2*t^6. + 3*t^6.175 + 3*t^6.201 + t^6.403 + 2*t^6.551 + 2*t^6.577 + t^6.604 + t^6.752 + 2*t^6.778 + 2*t^6.953 + t^6.98 + t^7.128 + 2*t^7.154 + t^7.181 + t^7.329 + 3*t^7.356 + t^7.382 + 3*t^7.53 + 2*t^7.557 + t^7.705 + 2*t^7.732 + 3*t^7.933 + 2*t^7.96 + t^8.081 + 2*t^8.108 - 2*t^8.134 + 5*t^8.309 + 2*t^8.335 + t^8.483 - 4*t^8.51 + 2*t^8.537 + 4*t^8.685 + 3*t^8.711 + t^8.738 + t^8.886 - t^8.913 - t^4.356/y - t^6.49/y - t^6.866/y + (2*t^7.644)/y + t^7.846/y + t^8.02/y + t^8.047/y + (2*t^8.222)/y + (3*t^8.423)/y + (2*t^8.597)/y - t^8.624/y + (3*t^8.799)/y + t^8.825/y - t^4.356*y - t^6.49*y - t^6.866*y + 2*t^7.644*y + t^7.846*y + t^8.02*y + t^8.047*y + 2*t^8.222*y + 3*t^8.423*y + 2*t^8.597*y - t^8.624*y + 3*t^8.799*y + t^8.825*y | t^2.134/g1^12 + 2*g1^14*t^2.51 + t^2.913/g1^22 + g1^22*t^3.087 + g1^4*t^3.289 + g1^30*t^3.665 + t^3.691/g1^32 + g1^56*t^4.04 + t^4.067/g1^6 + (2*t^4.268)/g1^24 + g1^20*t^4.443 + 2*g1^2*t^4.644 + t^4.846/g1^16 + 3*g1^28*t^5.02 + t^5.047/g1^34 + g1^10*t^5.222 + (2*t^5.423)/g1^8 + g1^36*t^5.597 + 3*g1^18*t^5.799 + t^5.825/g1^44 - 2*t^6. + 3*g1^44*t^6.175 + (3*t^6.201)/g1^18 + t^6.403/g1^36 + 2*g1^70*t^6.551 + 2*g1^8*t^6.577 + t^6.604/g1^54 + g1^52*t^6.752 + (2*t^6.778)/g1^10 + 2*g1^34*t^6.953 + t^6.98/g1^28 + g1^78*t^7.128 + 2*g1^16*t^7.154 + t^7.181/g1^46 + g1^60*t^7.329 + (3*t^7.356)/g1^2 + t^7.382/g1^64 + 3*g1^42*t^7.53 + (2*t^7.557)/g1^20 + g1^86*t^7.705 + 2*g1^24*t^7.732 + 3*g1^6*t^7.933 + (2*t^7.96)/g1^56 + g1^112*t^8.081 + 2*g1^50*t^8.108 - (2*t^8.134)/g1^12 + 5*g1^32*t^8.309 + (2*t^8.335)/g1^30 + g1^76*t^8.483 - 4*g1^14*t^8.51 + (2*t^8.537)/g1^48 + 4*g1^58*t^8.685 + (3*t^8.711)/g1^4 + t^8.738/g1^66 + g1^40*t^8.886 - t^8.913/g1^22 - t^4.356/(g1^2*y) - t^6.49/(g1^14*y) - (g1^12*t^6.866)/y + (2*g1^2*t^7.644)/y + t^7.846/(g1^16*y) + (g1^28*t^8.02)/y + t^8.047/(g1^34*y) + (2*g1^10*t^8.222)/y + (3*t^8.423)/(g1^8*y) + (2*g1^36*t^8.597)/y - t^8.624/(g1^26*y) + (3*g1^18*t^8.799)/y + t^8.825/(g1^44*y) - (t^4.356*y)/g1^2 - (t^6.49*y)/g1^14 - g1^12*t^6.866*y + 2*g1^2*t^7.644*y + (t^7.846*y)/g1^16 + g1^28*t^8.02*y + (t^8.047*y)/g1^34 + 2*g1^10*t^8.222*y + (3*t^8.423*y)/g1^8 + 2*g1^36*t^8.597*y - (t^8.624*y)/g1^26 + 3*g1^18*t^8.799*y + (t^8.825*y)/g1^44 |
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 |
|---|---|---|---|---|---|---|---|---|---|
| 55901 | SU2adj1nf2 | ${}M_{1}\phi_{1}^{2}$ + ${ }M_{2}q_{1}q_{2}$ + ${ }M_{3}q_{1}\tilde{q}_{1}$ + ${ }M_{4}q_{2}\tilde{q}_{1}$ + ${ }\phi_{1}\tilde{q}_{2}^{2}$ + ${ }M_{2}M_{4}$ + ${ }M_{5}q_{1}\tilde{q}_{2}$ + ${ }M_{3}M_{5}$ + ${ }M_{3}M_{6}$ | 0.6513 | 0.7969 | 0.8172 | [M:[1.0957, 1.0262, 1.1651, 0.9738, 0.8349, 0.8349], q:[0.3912, 0.5826], qb:[0.4437, 0.7739], phi:[0.4522]] | 2*t^2.505 + t^2.921 + t^3.079 + t^3.287 + t^3.653 + t^3.704 + t^3.861 + t^4.019 + t^4.069 + t^4.278 + t^4.435 + t^4.852 + 3*t^5.009 + t^5.426 + t^5.583 + 2*t^5.792 - 2*t^6. - t^4.356/y - t^4.356*y | detail |