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 |
|---|---|---|---|---|---|---|---|---|---|
| 56234 | 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_1^2$ + $ M_2M_5$ + $ M_2M_6$ + $ M_7\phi_1q_1\tilde{q}_1$ | 0.6935 | 0.887 | 0.7819 | [X:[], M:[1.1164, 1.1639, 0.8836, 0.6983, 0.8361, 0.8361, 0.6983], q:[0.3492, 0.5345], qb:[0.487, 0.7672], phi:[0.4655]] | [X:[], M:[[-1], [-10], [1], [-6], [10], [10], [-6]], q:[[-3], [4]], qb:[[13], [2]], phi:[[-4]]] | 1 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| $M_4$, $ M_7$, $ M_5$, $ M_6$, $ M_3$, $ \phi_1^2$, $ q_2\tilde{q}_1$, $ M_1$, $ \tilde{q}_1\tilde{q}_2$, $ \phi_1q_1q_2$, $ M_4^2$, $ M_4M_7$, $ M_7^2$, $ \phi_1\tilde{q}_1^2$, $ \phi_1q_2\tilde{q}_1$, $ M_4M_5$, $ M_4M_6$, $ M_5M_7$, $ M_6M_7$, $ \phi_1q_2^2$, $ M_3M_4$, $ M_3M_7$, $ \phi_1q_1\tilde{q}_2$, $ M_4\phi_1^2$, $ M_7\phi_1^2$, $ M_5^2$, $ M_5M_6$, $ M_6^2$, $ M_3M_5$, $ M_3M_6$, $ M_4q_2\tilde{q}_1$, $ M_7q_2\tilde{q}_1$, $ \phi_1\tilde{q}_1\tilde{q}_2$, $ M_3^2$, $ M_5\phi_1^2$, $ M_6\phi_1^2$, $ \phi_1q_2\tilde{q}_2$, $ M_1M_4$, $ M_1M_7$, $ M_3\phi_1^2$, $ M_5q_2\tilde{q}_1$, $ M_6q_2\tilde{q}_1$, $ M_3q_2\tilde{q}_1$, $ M_1M_5$, $ M_1M_6$, $ \phi_1^2q_2\tilde{q}_1$, $ M_4\tilde{q}_1\tilde{q}_2$, $ M_7\tilde{q}_1\tilde{q}_2$ | . | -2 | 2*t^2.09 + 2*t^2.51 + t^2.65 + t^2.79 + t^3.06 + t^3.35 + t^3.76 + t^4.05 + 3*t^4.19 + t^4.32 + t^4.46 + 5*t^4.6 + 2*t^4.75 + 2*t^4.89 + 3*t^5.02 + 4*t^5.16 + 3*t^5.3 + 2*t^5.44 + 2*t^5.57 + t^5.72 + 4*t^5.86 - 2*t^6. + t^6.13 + t^6.14 + 2*t^6.27 + 4*t^6.28 + 2*t^6.41 + 2*t^6.56 + 7*t^6.7 + 3*t^6.83 + 2*t^6.84 + 2*t^6.97 + 2*t^6.98 + 10*t^7.11 + 5*t^7.25 + t^7.38 + 5*t^7.4 + 5*t^7.53 + 2*t^7.54 + 7*t^7.67 + 4*t^7.81 + 5*t^7.95 + 4*t^8.08 - 4*t^8.09 + 4*t^8.22 + 7*t^8.37 + 5*t^8.38 - 3*t^8.51 + 3*t^8.64 - t^8.65 + 5*t^8.78 + 5*t^8.79 + 7*t^8.92 + t^8.94 - t^4.4/y - (2*t^6.49)/y - t^6.91/y + (5*t^7.6)/y + (2*t^7.75)/y + (3*t^7.89)/y + t^8.02/y + (4*t^8.16)/y + (4*t^8.3)/y + (3*t^8.44)/y + (2*t^8.57)/y - (3*t^8.59)/y + t^8.72/y + (5*t^8.86)/y - t^4.4*y - 2*t^6.49*y - t^6.91*y + 5*t^7.6*y + 2*t^7.75*y + 3*t^7.89*y + t^8.02*y + 4*t^8.16*y + 4*t^8.3*y + 3*t^8.44*y + 2*t^8.57*y - 3*t^8.59*y + t^8.72*y + 5*t^8.86*y | (2*t^2.09)/g1^6 + 2*g1^10*t^2.51 + g1*t^2.65 + t^2.79/g1^8 + g1^17*t^3.06 + t^3.35/g1 + g1^15*t^3.76 + t^4.05/g1^3 + (3*t^4.19)/g1^12 + g1^22*t^4.32 + g1^13*t^4.46 + 5*g1^4*t^4.6 + (2*t^4.75)/g1^5 + (2*t^4.89)/g1^14 + 3*g1^20*t^5.02 + 4*g1^11*t^5.16 + 3*g1^2*t^5.3 + (2*t^5.44)/g1^7 + 2*g1^27*t^5.57 + g1^18*t^5.72 + 4*g1^9*t^5.86 - 2*t^6. + g1^34*t^6.13 + t^6.14/g1^9 + 2*g1^25*t^6.27 + (4*t^6.28)/g1^18 + 2*g1^16*t^6.41 + 2*g1^7*t^6.56 + (7*t^6.7)/g1^2 + 3*g1^32*t^6.83 + (2*t^6.84)/g1^11 + 2*g1^23*t^6.97 + (2*t^6.98)/g1^20 + 10*g1^14*t^7.11 + 5*g1^5*t^7.25 + g1^39*t^7.38 + (5*t^7.4)/g1^4 + 5*g1^30*t^7.53 + (2*t^7.54)/g1^13 + 7*g1^21*t^7.67 + 4*g1^12*t^7.81 + 5*g1^3*t^7.95 + 4*g1^37*t^8.08 - (4*t^8.09)/g1^6 + 4*g1^28*t^8.22 + 7*g1^19*t^8.37 + (5*t^8.38)/g1^24 - 3*g1^10*t^8.51 + 3*g1^44*t^8.64 - g1*t^8.65 + 5*g1^35*t^8.78 + (5*t^8.79)/g1^8 + 7*g1^26*t^8.92 + t^8.94/g1^17 - t^4.4/(g1^4*y) - (2*t^6.49)/(g1^10*y) - (g1^6*t^6.91)/y + (5*g1^4*t^7.6)/y + (2*t^7.75)/(g1^5*y) + (3*t^7.89)/(g1^14*y) + (g1^20*t^8.02)/y + (4*g1^11*t^8.16)/y + (4*g1^2*t^8.3)/y + (3*t^8.44)/(g1^7*y) + (2*g1^27*t^8.57)/y - (3*t^8.59)/(g1^16*y) + (g1^18*t^8.72)/y + (5*g1^9*t^8.86)/y - (t^4.4*y)/g1^4 - (2*t^6.49*y)/g1^10 - g1^6*t^6.91*y + 5*g1^4*t^7.6*y + (2*t^7.75*y)/g1^5 + (3*t^7.89*y)/g1^14 + g1^20*t^8.02*y + 4*g1^11*t^8.16*y + 4*g1^2*t^8.3*y + (3*t^8.44*y)/g1^7 + 2*g1^27*t^8.57*y - (3*t^8.59*y)/g1^16 + g1^18*t^8.72*y + 5*g1^9*t^8.86*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 |
|---|---|---|---|---|---|---|---|---|---|
| 50977 | 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_1^2$ + $ M_2M_5$ + $ M_2M_6$ | 0.673 | 0.8479 | 0.7937 | [X:[], M:[1.1166, 1.1662, 0.8834, 0.6997, 0.8338, 0.8338], q:[0.3499, 0.5335], qb:[0.4839, 0.7668], phi:[0.4665]] | t^2.1 + 2*t^2.5 + t^2.65 + t^2.8 + t^3.05 + t^3.35 + t^3.75 + t^3.9 + t^4.05 + t^4.2 + t^4.3 + t^4.45 + 3*t^4.6 + t^4.75 + t^4.9 + 3*t^5. + 3*t^5.15 + 3*t^5.3 + t^5.45 + 2*t^5.55 + t^5.7 + 3*t^5.85 - t^6. - t^4.4/y - t^4.4*y | detail |