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 |
|---|---|---|---|---|---|---|---|---|---|
| 55453 | SU2adj1nf2 | $M_1q_1q_2$ + $ M_2q_1\tilde{q}_1$ + $ \phi_1q_1^2$ + $ M_3q_1\tilde{q}_2$ + $ M_3^2$ + $ M_4\phi_1q_2\tilde{q}_2$ + $ q_2^2\tilde{q}_1\tilde{q}_2$ + $ M_1X_1$ + $ M_2M_5$ + $ M_6\phi_1^2$ | 0.5917 | 0.7509 | 0.788 | [X:[1.3867], M:[0.6133, 0.6977, 1.0, 0.6889, 1.3023, 1.0756], q:[0.7689, 0.6178], qb:[0.5334, 0.2311], phi:[0.4622]] | [X:[[6]], M:[[-6], [16], [0], [-10], [-16], [-4]], q:[[-1], [7]], qb:[[-15], [1]], phi:[[2]]] | 1 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| $M_4$, $ \tilde{q}_1\tilde{q}_2$, $ q_2\tilde{q}_2$, $ \phi_1\tilde{q}_2^2$, $ M_3$, $ M_6$, $ q_2\tilde{q}_1$, $ \phi_1\tilde{q}_1\tilde{q}_2$, $ M_5$, $ M_4^2$, $ X_1$, $ M_4\tilde{q}_1\tilde{q}_2$, $ \phi_1\tilde{q}_1^2$, $ \tilde{q}_1^2\tilde{q}_2^2$, $ M_4q_2\tilde{q}_2$, $ \phi_1q_2\tilde{q}_1$, $ M_4\phi_1\tilde{q}_2^2$, $ q_2\tilde{q}_1\tilde{q}_2^2$, $ M_3M_4$, $ \phi_1\tilde{q}_1\tilde{q}_2^3$, $ \phi_1q_2^2$, $ q_2^2\tilde{q}_2^2$, $ M_4M_6$, $ \phi_1q_1\tilde{q}_1$, $ M_3\tilde{q}_1\tilde{q}_2$, $ \phi_1q_2\tilde{q}_2^3$, $ M_4q_2\tilde{q}_1$, $ M_6\tilde{q}_1\tilde{q}_2$, $ \phi_1q_1q_2$, $ M_3q_2\tilde{q}_2$, $ \phi_1^2\tilde{q}_2^4$, $ M_4\phi_1\tilde{q}_1\tilde{q}_2$, $ q_2\tilde{q}_1^2\tilde{q}_2$, $ M_6q_2\tilde{q}_2$, $ M_3\phi_1\tilde{q}_2^2$, $ M_4M_5$, $ \phi_1\tilde{q}_1^2\tilde{q}_2^2$ | $M_6\phi_1\tilde{q}_2^2$ | -1 | t^2.07 + t^2.29 + t^2.55 + t^2.77 + t^3. + t^3.23 + t^3.45 + t^3.68 + t^3.91 + t^4.13 + t^4.16 + t^4.36 + 2*t^4.59 + t^4.61 + 2*t^4.84 + 2*t^5.07 + t^5.09 + 2*t^5.29 + t^5.32 + 2*t^5.52 + 2*t^5.55 + t^5.75 + t^5.77 + 2*t^5.97 - t^6. + 2*t^6.2 + 2*t^6.23 - t^6.25 + t^6.43 + 3*t^6.45 - t^6.48 + 2*t^6.65 + 2*t^6.68 + 2*t^6.88 + 3*t^6.91 - t^6.93 + 4*t^7.13 + 5*t^7.36 + 4*t^7.59 + t^7.61 + 3*t^7.81 + 2*t^7.84 + 3*t^8.04 + t^8.09 + 4*t^8.27 + t^8.32 + 3*t^8.49 + 2*t^8.52 - 3*t^8.55 + 2*t^8.72 + 5*t^8.75 - 3*t^8.77 + 2*t^8.95 + 3*t^8.97 - t^4.39/y - t^6.45/y + t^7.36/y + t^7.61/y + (2*t^7.84)/y + (2*t^8.07)/y + (2*t^8.29)/y + (2*t^8.32)/y + t^8.52/y + t^8.55/y + (2*t^8.75)/y + (2*t^8.77)/y + (2*t^8.97)/y - t^4.39*y - t^6.45*y + t^7.36*y + t^7.61*y + 2*t^7.84*y + 2*t^8.07*y + 2*t^8.29*y + 2*t^8.32*y + t^8.52*y + t^8.55*y + 2*t^8.75*y + 2*t^8.77*y + 2*t^8.97*y | t^2.07/g1^10 + t^2.29/g1^14 + g1^8*t^2.55 + g1^4*t^2.77 + t^3. + t^3.23/g1^4 + t^3.45/g1^8 + t^3.68/g1^12 + t^3.91/g1^16 + t^4.13/g1^20 + g1^6*t^4.16 + t^4.36/g1^24 + (2*t^4.59)/g1^28 + t^4.61/g1^2 + (2*t^4.84)/g1^6 + (2*t^5.07)/g1^10 + g1^16*t^5.09 + (2*t^5.29)/g1^14 + g1^12*t^5.32 + (2*t^5.52)/g1^18 + 2*g1^8*t^5.55 + t^5.75/g1^22 + g1^4*t^5.77 + (2*t^5.97)/g1^26 - t^6. + (2*t^6.2)/g1^30 + (2*t^6.23)/g1^4 - g1^22*t^6.25 + t^6.43/g1^34 + (3*t^6.45)/g1^8 - g1^18*t^6.48 + (2*t^6.65)/g1^38 + (2*t^6.68)/g1^12 + (2*t^6.88)/g1^42 + (3*t^6.91)/g1^16 - g1^10*t^6.93 + (4*t^7.13)/g1^20 + (5*t^7.36)/g1^24 + (4*t^7.59)/g1^28 + t^7.61/g1^2 + (3*t^7.81)/g1^32 + (2*t^7.84)/g1^6 + (3*t^8.04)/g1^36 + g1^16*t^8.09 + (4*t^8.27)/g1^40 + g1^12*t^8.32 + (3*t^8.49)/g1^44 + (2*t^8.52)/g1^18 - 3*g1^8*t^8.55 + (2*t^8.72)/g1^48 + (5*t^8.75)/g1^22 - 3*g1^4*t^8.77 + (2*t^8.95)/g1^52 + (3*t^8.97)/g1^26 - (g1^2*t^4.39)/y - t^6.45/(g1^8*y) + t^7.36/(g1^24*y) + t^7.61/(g1^2*y) + (2*t^7.84)/(g1^6*y) + (2*t^8.07)/(g1^10*y) + (2*t^8.29)/(g1^14*y) + (2*g1^12*t^8.32)/y + t^8.52/(g1^18*y) + (g1^8*t^8.55)/y + (2*t^8.75)/(g1^22*y) + (2*g1^4*t^8.77)/y + (2*t^8.97)/(g1^26*y) - g1^2*t^4.39*y - (t^6.45*y)/g1^8 + (t^7.36*y)/g1^24 + (t^7.61*y)/g1^2 + (2*t^7.84*y)/g1^6 + (2*t^8.07*y)/g1^10 + (2*t^8.29*y)/g1^14 + 2*g1^12*t^8.32*y + (t^8.52*y)/g1^18 + g1^8*t^8.55*y + (2*t^8.75*y)/g1^22 + 2*g1^4*t^8.77*y + (2*t^8.97*y)/g1^26 |
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 |
|---|---|---|---|---|---|---|---|---|---|
| 47209 | SU2adj1nf2 | $M_1q_1q_2$ + $ M_2q_1\tilde{q}_1$ + $ \phi_1q_1^2$ + $ M_3q_1\tilde{q}_2$ + $ M_3^2$ + $ M_4\phi_1q_2\tilde{q}_2$ + $ q_2^2\tilde{q}_1\tilde{q}_2$ + $ M_1X_1$ + $ M_2M_5$ | 0.5988 | 0.7618 | 0.7861 | [X:[1.3822], M:[0.6178, 0.6859, 1.0, 0.6963, 1.3141], q:[0.7696, 0.6126], qb:[0.5445, 0.2304], phi:[0.4607]] | t^2.09 + t^2.32 + t^2.53 + 2*t^2.76 + t^3. + t^3.47 + t^3.71 + t^3.94 + t^4.15 + t^4.18 + t^4.41 + t^4.62 + 2*t^4.65 + 3*t^4.85 + t^5.06 + 3*t^5.09 + 2*t^5.29 + t^5.32 + 4*t^5.53 + t^5.56 + t^5.76 + t^5.8 - 2*t^6. - t^4.38/y - t^4.38*y | detail |