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 |
|---|---|---|---|---|---|---|---|---|---|
| 56005 | SU2adj1nf2 | $M_1q_1q_2$ + $ M_2q_1\tilde{q}_1$ + $ M_3q_1\tilde{q}_2$ + $ M_4q_2\tilde{q}_2$ + $ M_1M_3$ + $ \phi_1\tilde{q}_2^2$ + $ M_5\phi_1q_1q_2$ + $ M_4M_6$ + $ \tilde{q}_1\tilde{q}_2$ + $ M_2X_1$ + $ \phi_1^2X_2$ | 0.4367 | 0.512 | 0.8529 | [X:[1.5066, 1.3974], M:[1.2053, 0.4934, 0.7947, 0.7119, 0.904, 1.2881], q:[0.3559, 0.4388], qb:[1.1507, 0.8493], phi:[0.3013]] | [X:[[-10], [4]], M:[[-8], [10], [8], [-18], [-6], [18]], q:[[-9], [17]], qb:[[-1], [1]], phi:[[-2]]] | 1 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| $M_3$, $ M_5$, $ \phi_1q_1^2$, $ \phi_1q_2^2$, $ X_2$, $ M_3^2$, $ q_2\tilde{q}_1$, $ \phi_1q_2\tilde{q}_2$, $ M_3M_5$, $ M_2^2q_1^2$, $ M_5^2$, $ \phi_1q_1\tilde{q}_1$, $ M_3\phi_1q_2^2$ | . | -2 | t^2.38 + t^2.71 + t^3.04 + t^3.54 + t^4.19 + t^4.77 + t^5.1 + 2*t^5.42 + t^5.92 - 2*t^6. + t^6.08 + t^6.58 - t^6.66 + t^7.07 + 2*t^7.81 + t^8.14 + t^8.31 - 2*t^8.38 + t^8.46 - t^8.71 + t^8.96 - t^3.9/y - t^6.62/y + t^7.19/y + t^8.1/y + t^8.42/y + t^8.75/y + t^8.92/y - t^3.9*y - t^6.62*y + t^7.19*y + t^8.1*y + t^8.42*y + t^8.75*y + t^8.92*y | g1^8*t^2.38 + t^2.71/g1^6 + t^3.04/g1^20 + g1^32*t^3.54 + g1^4*t^4.19 + g1^16*t^4.77 + g1^2*t^5.1 + (2*t^5.42)/g1^12 + g1^40*t^5.92 - 2*t^6. + t^6.08/g1^40 + g1^12*t^6.58 - t^6.66/g1^28 + g1^64*t^7.07 + (2*t^7.81)/g1^4 + t^8.14/g1^18 + g1^48*t^8.31 - 2*g1^8*t^8.38 + t^8.46/g1^32 - t^8.71/g1^6 + g1^20*t^8.96 - t^3.9/(g1^2*y) - t^6.62/(g1^8*y) + (g1^4*t^7.19)/y + (g1^2*t^8.1)/y + t^8.42/(g1^12*y) + t^8.75/(g1^26*y) + (g1^40*t^8.92)/y - (t^3.9*y)/g1^2 - (t^6.62*y)/g1^8 + g1^4*t^7.19*y + g1^2*t^8.1*y + (t^8.42*y)/g1^12 + (t^8.75*y)/g1^26 + g1^40*t^8.92*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 |
|---|---|---|---|---|---|---|---|---|---|
| 48307 | SU2adj1nf2 | $M_1q_1q_2$ + $ M_2q_1\tilde{q}_1$ + $ M_3q_1\tilde{q}_2$ + $ M_4q_2\tilde{q}_2$ + $ M_1M_3$ + $ \phi_1\tilde{q}_2^2$ + $ M_5\phi_1q_1q_2$ + $ M_4M_6$ | 0.6637 | 0.8211 | 0.8083 | [X:[], M:[1.168, 1.0146, 0.832, 0.7862, 0.7178, 1.2138], q:[0.3931, 0.4389], qb:[0.5922, 0.7749], phi:[0.4502]] | t^2.15 + t^2.5 + t^2.7 + t^3.04 + t^3.09 + t^3.5 + t^3.64 + t^3.71 + t^3.98 + t^4.1 + 2*t^4.31 + t^4.44 + t^4.65 + t^4.85 + t^4.9 + t^4.99 + 2*t^5.2 + t^5.25 + t^5.59 + t^5.66 + t^5.75 + 2*t^5.79 - 2*t^6. - t^4.35/y - t^4.35*y | detail |