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 |
|---|---|---|---|---|---|---|---|---|---|
| 46594 | SU2adj1nf2 | $M_1q_1q_2$ + $ M_2q_1\tilde{q}_1$ + $ \phi_1q_1\tilde{q}_2$ + $ M_1M_2$ + $ M_3\phi_1\tilde{q}_1^2$ + $ M_3^2$ + $ q_2^2\tilde{q}_1^2$ + $ \phi_1^2X_1$ | 0.474 | 0.5573 | 0.8505 | [X:[1.3333], M:[0.8333, 1.1667, 1.0], q:[0.5, 0.6667], qb:[0.3333, 1.1667], phi:[0.3333]] | [X:[[0]], M:[[0], [0], [0]], q:[[0], [0]], qb:[[0], [0]], phi:[[0]]] | 0 | {a: 91/192, c: 107/192, X1: 4/3, M1: 5/6, M2: 7/6, M3: 1, q1: 1/2, q2: 2/3, qb1: 1/3, qb2: 7/6, phi1: 1/3} |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| $M_1$, $ M_3$, $ q_2\tilde{q}_1$, $ M_2$, $ \phi_1q_2\tilde{q}_1$, $ X_1$, $ M_1^2$, $ \phi_1q_2^2$, $ q_1\tilde{q}_2$, $ M_1M_3$, $ q_2\tilde{q}_2$, $ \phi_1\tilde{q}_1\tilde{q}_2$ | $M_3q_2\tilde{q}_1$ | 0 | t^2.5 + 2*t^3. + t^3.5 + 2*t^4. + 2*t^5. + t^5.5 + t^6.5 + t^7. + t^7.5 + 3*t^8. - t^4./y + (2*t^8.5)/y - t^4.*y + 2*t^8.5*y | t^2.5 + 2*t^3. + t^3.5 + 2*t^4. + 2*t^5. + t^5.5 + t^6.5 + t^7. + t^7.5 + 3*t^8. - t^4./y + (2*t^8.5)/y - t^4.*y + 2*t^8.5*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 |
|---|---|---|---|---|---|---|---|---|
| 47130 | $M_1q_1q_2$ + $ M_2q_1\tilde{q}_1$ + $ \phi_1q_1\tilde{q}_2$ + $ M_1M_2$ + $ M_3\phi_1\tilde{q}_1^2$ + $ M_3^2$ + $ q_2^2\tilde{q}_1^2$ + $ \phi_1^2X_1$ + $ M_2M_4$ | 0.4883 | 0.582 | 0.8389 | [X:[1.3333], M:[0.8333, 1.1667, 1.0, 0.8333], q:[0.5, 0.6667], qb:[0.3333, 1.1667], phi:[0.3333]] | 2*t^2.5 + 2*t^3. + 2*t^4. + 4*t^5. + 3*t^5.5 - t^6. - t^4./y - t^4.*y | detail | {a: 125/256, c: 149/256, X1: 4/3, M1: 5/6, M2: 7/6, M3: 1, M4: 5/6, q1: 1/2, q2: 2/3, qb1: 1/3, qb2: 7/6, phi1: 1/3} |
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 |
|---|---|---|---|---|---|---|---|---|---|
| 46322 | SU2adj1nf2 | $M_1q_1q_2$ + $ M_2q_1\tilde{q}_1$ + $ \phi_1q_1\tilde{q}_2$ + $ M_1M_2$ + $ M_3\phi_1\tilde{q}_1^2$ + $ M_3^2$ | 0.5526 | 0.6831 | 0.809 | [X:[], M:[0.9176, 1.0824, 1.0], q:[0.6264, 0.456], qb:[0.2912, 0.956], phi:[0.4176]] | t^2.24 + t^2.51 + t^2.75 + t^3. + t^3.25 + t^3.49 + t^3.74 + t^3.99 + t^4.24 + t^4.48 + 2*t^4.75 + t^4.99 + t^5.01 + t^5.24 + t^5.49 + t^5.51 + t^5.74 + t^5.75 + t^5.98 - t^4.25/y - t^4.25*y | detail |