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 |
|---|---|---|---|---|---|---|---|---|---|
| 448 | SU2adj1nf2 | $\phi_1q_1^2$ + $ q_1q_2$ + $ \phi_1^2X_1$ + $ M_1\phi_1\tilde{q}_1\tilde{q}_2$ + $ M_2\phi_1\tilde{q}_1^2$ + $ M_1M_2$ + $ \tilde{q}_1^2\tilde{q}_2^2$ + $ M_2M_3$ | 0.3662 | 0.4287 | 0.8542 | [X:[1.5], M:[0.75, 1.25, 0.75], q:[0.875, 1.125], qb:[0.25, 0.75], phi:[0.25]] | [X:[[0]], M:[[0], [0], [0]], q:[[0], [0]], qb:[[0], [0]], phi:[[0]]] | 0 | {a: 375/1024, c: 439/1024, X1: 3/2, M1: 3/4, M2: 5/4, M3: 3/4, q1: 7/8, q2: 9/8, qb1: 1/4, qb2: 3/4, phi1: 1/4} |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| $M_1$, $ M_3$, $ \tilde{q}_1\tilde{q}_2$, $ M_1^2$, $ M_1M_3$, $ M_3^2$, $ X_1$, $ M_1\tilde{q}_1\tilde{q}_2$, $ M_3\tilde{q}_1\tilde{q}_2$, $ \phi_1\tilde{q}_2^2$ | . | -1 | 2*t^2.25 + t^3. + 3*t^4.5 + 2*t^5.25 - t^6. + 2*t^6.75 + 2*t^7.5 - 2*t^8.25 - t^3.75/y - t^6./y + (2*t^7.5)/y + t^8.25/y - t^3.75*y - t^6.*y + 2*t^7.5*y + t^8.25*y | 2*t^2.25 + t^3. + 3*t^4.5 + 2*t^5.25 - t^6. + 2*t^6.75 + 2*t^7.5 - 2*t^8.25 - t^3.75/y - t^6./y + (2*t^7.5)/y + t^8.25/y - t^3.75*y - t^6.*y + 2*t^7.5*y + t^8.25*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 |
|---|---|---|---|---|---|---|---|---|---|
| 33 | SU2adj1nf1 | $\phi_1^2X_1$ + $ M_1\phi_1q_1^2$ + $ M_2\phi_1q_1\tilde{q}_1$ + $ M_1M_2$ + $ q_1^2\tilde{q}_1^2$ + $ M_1M_3$ | 0.3662 | 0.4287 | 0.8542 | [X:[1.5], M:[1.25, 0.75, 0.75], q:[0.25], qb:[0.75], phi:[0.25]] | 2*t^2.25 + t^3. + 3*t^4.5 + 2*t^5.25 - t^6. - t^3.75/y - t^6./y - t^3.75*y - t^6.*y | detail | {a: 375/1024, c: 439/1024, X1: 3/2, M1: 5/4, M2: 3/4, M3: 3/4, q1: 1/4, qb1: 3/4, phi1: 1/4} |
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 |
|---|---|---|---|---|---|---|---|---|---|
| 275 | SU2adj1nf2 | $\phi_1q_1^2$ + $ q_1q_2$ + $ \phi_1^2X_1$ + $ M_1\phi_1\tilde{q}_1\tilde{q}_2$ + $ M_2\phi_1\tilde{q}_1^2$ + $ M_1M_2$ + $ \tilde{q}_1^2\tilde{q}_2^2$ | 0.3472 | 0.394 | 0.881 | [X:[1.5], M:[0.75, 1.25], q:[0.875, 1.125], qb:[0.25, 0.75], phi:[0.25]] | t^2.25 + t^3. + t^3.75 + t^4.5 + t^5.25 - t^3.75/y - t^3.75*y | detail | {a: 711/2048, c: 807/2048, X1: 3/2, M1: 3/4, M2: 5/4, q1: 7/8, q2: 9/8, qb1: 1/4, qb2: 3/4, phi1: 1/4} |