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 |
|---|---|---|---|---|---|---|---|---|---|
| 2708 | SU2adj1nf2 | $\phi_1q_1q_2$ + $ M_1q_1\tilde{q}_1$ + $ M_1^2$ + $ \phi_1\tilde{q}_1^3\tilde{q}_2$ + $ \phi_1\tilde{q}_2^2$ + $ \phi_1^2X_1$ + $ M_2q_2\tilde{q}_1$ | 0.4526 | 0.533 | 0.8492 | [X:[1.4286], M:[1.0, 0.7143], q:[0.7143, 1.0], qb:[0.2857, 0.8571], phi:[0.2857]] | [X:[[0]], M:[[0], [0]], q:[[0], [0]], qb:[[0], [0]], phi:[[0]]] | 0 | {a: 621/1372, c: 2925/5488, X1: 10/7, M1: 1, M2: 5/7, q1: 5/7, q2: 1, qb1: 2/7, qb2: 6/7, phi1: 2/7} |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| $M_2$, $ \phi_1\tilde{q}_1^2$, $ M_1$, $ \tilde{q}_1\tilde{q}_2$, $ M_2^2$, $ \phi_1\tilde{q}_1\tilde{q}_2$, $ X_1$, $ M_2\phi_1\tilde{q}_1^2$, $ q_1\tilde{q}_2$, $ M_1M_2$, $ q_1q_2$, $ M_1\phi_1\tilde{q}_1^2$, $ q_2\tilde{q}_2$, $ M_2\tilde{q}_1\tilde{q}_2$ | . | 0 | t^2.14 + t^2.57 + t^3. + t^3.43 + 2*t^4.29 + t^4.71 + 2*t^5.14 + t^5.57 + t^6.43 + t^6.86 + t^7.29 + 2*t^7.71 - t^8.14 + t^8.57 - t^3.86/y - t^6./y + (2*t^7.71)/y + (2*t^8.57)/y - t^3.86*y - t^6.*y + 2*t^7.71*y + 2*t^8.57*y | t^2.14 + t^2.57 + t^3. + t^3.43 + 2*t^4.29 + t^4.71 + 2*t^5.14 + t^5.57 + t^6.43 + t^6.86 + t^7.29 + 2*t^7.71 - t^8.14 + t^8.57 - t^3.86/y - t^6./y + (2*t^7.71)/y + (2*t^8.57)/y - t^3.86*y - t^6.*y + 2*t^7.71*y + 2*t^8.57*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 |
|---|---|---|---|---|---|---|---|---|
| 3215 | $\phi_1q_1q_2$ + $ M_1q_1\tilde{q}_1$ + $ M_1^2$ + $ \phi_1\tilde{q}_1^3\tilde{q}_2$ + $ \phi_1\tilde{q}_2^2$ + $ \phi_1^2X_1$ + $ M_2q_2\tilde{q}_1$ + $ M_3\tilde{q}_1\tilde{q}_2$ | 0.4652 | 0.5545 | 0.839 | [X:[1.4286], M:[1.0, 0.7143, 0.8571], q:[0.7143, 1.0], qb:[0.2857, 0.8571], phi:[0.2857]] | t^2.14 + 2*t^2.57 + t^3. + 2*t^4.29 + 2*t^4.71 + 4*t^5.14 + t^5.57 - t^6. - t^3.86/y - t^6./y - t^3.86*y - t^6.*y | detail | {a: 2553/5488, c: 3043/5488, X1: 10/7, M1: 1, M2: 5/7, M3: 6/7, q1: 5/7, q2: 1, qb1: 2/7, qb2: 6/7, phi1: 2/7} |
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 |
|---|---|---|---|---|---|---|---|---|---|
| 1711 | SU2adj1nf2 | $\phi_1q_1q_2$ + $ M_1q_1\tilde{q}_1$ + $ M_1^2$ + $ \phi_1\tilde{q}_1^3\tilde{q}_2$ + $ \phi_1\tilde{q}_2^2$ + $ \phi_1^2X_1$ | 0.4324 | 0.4949 | 0.8737 | [X:[1.4286], M:[1.0], q:[0.7143, 1.0], qb:[0.2857, 0.8571], phi:[0.2857]] | t^2.57 + t^3. + t^3.43 + t^3.86 + t^4.29 + t^5.14 - t^3.86/y - t^3.86*y | detail | {a: 339/784, c: 97/196, X1: 10/7, M1: 1, q1: 5/7, q2: 1, qb1: 2/7, qb2: 6/7, phi1: 2/7} |