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 |
|---|---|---|---|---|---|---|---|---|---|
| 3220 | SU2adj1nf2 | ${}\phi_{1}q_{1}^{2}$ + ${ }M_{1}q_{2}\tilde{q}_{1}$ + ${ }\phi_{1}^{4}$ + ${ }M_{2}\phi_{1}q_{2}\tilde{q}_{2}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }M_{3}\phi_{1}q_{2}^{2}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ | 0.629 | 0.7983 | 0.788 | [M:[1.0975, 0.75, 0.6949, 1.25], q:[0.75, 0.4025], qb:[0.5, 0.3475], phi:[0.5]] | [M:[[1], [0], [2], [0]], q:[[0], [-1]], qb:[[0], [1]], phi:[[0]]] | 1 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| ${}M_{3}$, ${ }M_{2}$, ${ }\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}^{2}$, ${ }M_{1}$, ${ }q_{1}\tilde{q}_{2}$, ${ }q_{1}q_{2}$, ${ }\phi_{1}\tilde{q}_{2}^{2}$, ${ }M_{4}$, ${ }q_{1}\tilde{q}_{1}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{3}^{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }M_{2}M_{3}$, ${ }M_{2}^{2}$, ${ }\phi_{1}\tilde{q}_{1}^{2}$, ${ }M_{3}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{3}\phi_{1}^{2}$, ${ }\tilde{q}_{1}^{2}\tilde{q}_{2}^{2}$, ${ }M_{2}\phi_{1}^{2}$, ${ }M_{1}M_{3}$, ${ }M_{3}q_{1}\tilde{q}_{2}$, ${ }M_{1}M_{2}$, ${ }M_{3}q_{1}q_{2}$, ${ }M_{2}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}^{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{3}\phi_{1}\tilde{q}_{2}^{2}$, ${ }M_{3}M_{4}$, ${ }M_{3}q_{1}\tilde{q}_{1}$, ${ }M_{2}\phi_{1}\tilde{q}_{2}^{2}$, ${ }q_{1}\tilde{q}_{1}\tilde{q}_{2}^{2}$ | ${}M_{2}M_{4}$ | 0 | t^2.085 + t^2.25 + t^2.542 + t^3. + 2*t^3.292 + t^3.458 + t^3.585 + 2*t^3.75 + t^4.042 + t^4.17 + t^4.208 + t^4.335 + 2*t^4.5 + t^4.627 + t^4.792 + 2*t^5.085 + t^5.25 + 2*t^5.377 + 3*t^5.542 + t^5.67 + 4*t^5.835 + 2*t^6.127 - t^6.165 + t^6.254 + 3*t^6.292 + t^6.42 - t^6.458 + 6*t^6.585 + t^6.712 + 3*t^6.75 + 3*t^6.877 + 4*t^7.042 + 3*t^7.17 - t^7.208 + 4*t^7.335 + 2*t^7.462 + 2*t^7.5 + 5*t^7.627 - t^7.665 + t^7.754 + 3*t^7.792 + 4*t^7.92 - t^7.958 + 3*t^8.085 + 2*t^8.212 - t^8.25 + t^8.339 + 5*t^8.377 - t^8.415 + t^8.504 - t^8.542 + 7*t^8.67 - 2*t^8.708 + t^8.797 + 5*t^8.835 + 3*t^8.962 - t^4.5/y - t^6.585/y + t^7.208/y + t^7.335/y + t^7.627/y + t^8.085/y + t^8.25/y + (2*t^8.377)/y + t^8.415/y + (4*t^8.542)/y + t^8.708/y + (5*t^8.835)/y - t^4.5*y - t^6.585*y + t^7.208*y + t^7.335*y + t^7.627*y + t^8.085*y + t^8.25*y + 2*t^8.377*y + t^8.415*y + 4*t^8.542*y + t^8.708*y + 5*t^8.835*y | g1^2*t^2.085 + t^2.25 + g1*t^2.542 + t^3. + 2*g1*t^3.292 + t^3.458/g1 + g1^2*t^3.585 + 2*t^3.75 + g1*t^4.042 + g1^4*t^4.17 + t^4.208/g1 + g1^2*t^4.335 + 2*t^4.5 + g1^3*t^4.627 + g1*t^4.792 + 2*g1^2*t^5.085 + t^5.25 + 2*g1^3*t^5.377 + 3*g1*t^5.542 + g1^4*t^5.67 + 4*g1^2*t^5.835 + 2*g1^3*t^6.127 - t^6.165/g1^2 + g1^6*t^6.254 + 3*g1*t^6.292 + g1^4*t^6.42 - t^6.458/g1 + 6*g1^2*t^6.585 + g1^5*t^6.712 + 3*t^6.75 + 3*g1^3*t^6.877 + 4*g1*t^7.042 + 3*g1^4*t^7.17 - t^7.208/g1 + 4*g1^2*t^7.335 + 2*g1^5*t^7.462 + 2*t^7.5 + 5*g1^3*t^7.627 - t^7.665/g1^2 + g1^6*t^7.754 + 3*g1*t^7.792 + 4*g1^4*t^7.92 - t^7.958/g1 + 3*g1^2*t^8.085 + 2*g1^5*t^8.212 - t^8.25 + g1^8*t^8.339 + 5*g1^3*t^8.377 - t^8.415/g1^2 + g1^6*t^8.504 - g1*t^8.542 + 7*g1^4*t^8.67 - (2*t^8.708)/g1 + g1^7*t^8.797 + 5*g1^2*t^8.835 + 3*g1^5*t^8.962 - t^4.5/y - (g1^2*t^6.585)/y + t^7.208/(g1*y) + (g1^2*t^7.335)/y + (g1^3*t^7.627)/y + (g1^2*t^8.085)/y + t^8.25/y + (2*g1^3*t^8.377)/y + t^8.415/(g1^2*y) + (4*g1*t^8.542)/y + t^8.708/(g1*y) + (5*g1^2*t^8.835)/y - t^4.5*y - g1^2*t^6.585*y + (t^7.208*y)/g1 + g1^2*t^7.335*y + g1^3*t^7.627*y + g1^2*t^8.085*y + t^8.25*y + 2*g1^3*t^8.377*y + (t^8.415*y)/g1^2 + 4*g1*t^8.542*y + (t^8.708*y)/g1 + 5*g1^2*t^8.835*y |
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 |
|---|---|---|---|---|---|---|---|---|---|
| 2711 | SU2adj1nf2 | ${}\phi_{1}q_{1}^{2}$ + ${ }M_{1}q_{2}\tilde{q}_{1}$ + ${ }\phi_{1}^{4}$ + ${ }M_{2}\phi_{1}q_{2}\tilde{q}_{2}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }M_{3}\phi_{1}q_{2}^{2}$ | 0.6481 | 0.8329 | 0.7781 | [M:[1.0975, 0.75, 0.6949], q:[0.75, 0.4025], qb:[0.5, 0.3475], phi:[0.5]] | t^2.085 + 2*t^2.25 + t^2.542 + t^3. + 2*t^3.292 + t^3.458 + t^3.585 + t^3.75 + t^4.042 + t^4.17 + t^4.208 + 2*t^4.335 + 4*t^4.5 + t^4.627 + 2*t^4.792 + 2*t^5.085 + 2*t^5.25 + 2*t^5.377 + 5*t^5.542 + t^5.67 + t^5.708 + 4*t^5.835 - t^4.5/y - t^4.5*y | detail |