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 |
|---|---|---|---|---|---|---|---|---|---|
| 381 | SU2adj1nf2 | $\phi_1q_1^2$ + $ \phi_1q_2^2$ + $ M_1q_1\tilde{q}_1$ + $ M_2\phi_1\tilde{q}_2^2$ + $ M_3\phi_1\tilde{q}_1^2$ + $ M_1M_3$ + $ M_2X_1$ + $ \tilde{q}_1^2\tilde{q}_2^2$ + $ \phi_1^2X_2$ | 0.5 | 0.5833 | 0.8571 | [X:[1.7778, 1.3333], M:[0.8889, 0.2222, 1.1111], q:[0.8333, 0.8333], qb:[0.2778, 0.7222], phi:[0.3333]] | [X:[[0], [0]], M:[[0], [0], [0]], q:[[0], [0]], qb:[[0], [0]], phi:[[0]]] | 0 | {a: 1/2, c: 7/12, X1: 16/9, X2: 4/3, M1: 8/9, M2: 2/9, M3: 10/9, q1: 5/6, q2: 5/6, qb1: 5/18, qb2: 13/18, phi1: 1/3} |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| $M_1$, $ \tilde{q}_1\tilde{q}_2$, $ M_3$, $ q_2\tilde{q}_1$, $ \phi_1\tilde{q}_1\tilde{q}_2$, $ X_2$, $ q_1\tilde{q}_2$, $ q_2\tilde{q}_2$, $ q_1q_2$ | $M_1q_2\tilde{q}_1$ | 0 | t^2.67 + t^3. + 2*t^3.33 + 2*t^4. + t^4.67 + t^5. + 2*t^6.67 + 2*t^7.33 + 4*t^8. - t^8.67 - t^4./y + t^8.67/y - t^4.*y + t^8.67*y | t^2.67 + t^3. + 2*t^3.33 + 2*t^4. + t^4.67 + t^5. + 2*t^6.67 + 2*t^7.33 + 4*t^8. - t^8.67 - t^4./y + t^8.67/y - t^4.*y + t^8.67*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 |
|---|---|---|---|---|---|---|---|---|
| 619 | $\phi_1q_1^2$ + $ \phi_1q_2^2$ + $ M_1q_1\tilde{q}_1$ + $ M_2\phi_1\tilde{q}_2^2$ + $ M_3\phi_1\tilde{q}_1^2$ + $ M_1M_3$ + $ M_2X_1$ + $ \tilde{q}_1^2\tilde{q}_2^2$ + $ \phi_1^2X_2$ + $ M_3M_4$ | 0.51 | 0.6003 | 0.8496 | [X:[1.7778, 1.3333], M:[0.8889, 0.2222, 1.1111, 0.8889], q:[0.8333, 0.8333], qb:[0.2778, 0.7222], phi:[0.3333]] | 2*t^2.67 + t^3. + t^3.33 + 2*t^4. + t^4.67 + t^5. + 2*t^5.33 + t^5.67 - t^4./y - t^4.*y | detail | {a: 661/1296, c: 389/648, X1: 16/9, X2: 4/3, M1: 8/9, M2: 2/9, M3: 10/9, M4: 8/9, q1: 5/6, q2: 5/6, qb1: 5/18, qb2: 13/18, 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 |
|---|---|---|---|---|---|---|---|---|---|
| 241 | SU2adj1nf2 | $\phi_1q_1^2$ + $ \phi_1q_2^2$ + $ M_1q_1\tilde{q}_1$ + $ M_2\phi_1\tilde{q}_2^2$ + $ M_3\phi_1\tilde{q}_1^2$ + $ M_1M_3$ + $ M_2X_1$ | 0.5614 | 0.6887 | 0.8152 | [X:[1.4324], M:[0.9382, 0.5676, 1.0618], q:[0.7963, 0.7963], qb:[0.2654, 0.5125], phi:[0.4073]] | t^2.33 + t^2.44 + t^2.81 + 2*t^3.19 + t^3.56 + 2*t^3.93 + t^4.3 + t^4.67 + 2*t^4.78 + t^4.89 + t^5.15 + 2*t^5.52 + t^5.63 + t^5.89 - t^4.22/y - t^4.22*y | detail |