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 |
|---|---|---|---|---|---|---|---|---|---|
| 56204 | 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$ + $ M_5q_2\tilde{q}_1$ + $ \phi_1\tilde{q}_2^2$ + $ M_4\phi_1q_1^2$ + $ M_6\phi_1q_1q_2$ + $ M_1M_7$ | 0.7013 | 0.8858 | 0.7917 | [X:[], M:[1.1717, 0.9701, 0.8283, 0.7811, 0.9228, 0.7339, 0.8283], q:[0.3906, 0.4378], qb:[0.6394, 0.7811], phi:[0.4378]] | [X:[], M:[[3], [-18], [-3], [2], [-13], [7], [-3]], q:[[1], [-4]], qb:[[17], [2]], phi:[[-4]]] | 1 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| $M_6$, $ M_4$, $ M_3$, $ M_7$, $ \phi_1^2$, $ M_5$, $ M_2$, $ \phi_1q_1^2$, $ \phi_1q_2^2$, $ \tilde{q}_1\tilde{q}_2$, $ M_6^2$, $ \phi_1q_1\tilde{q}_1$, $ M_4M_6$, $ \phi_1q_2\tilde{q}_1$, $ M_4^2$, $ M_3M_6$, $ M_6M_7$, $ M_3M_4$, $ M_4M_7$, $ M_6\phi_1^2$, $ \phi_1q_1\tilde{q}_2$, $ M_3^2$, $ M_5M_6$, $ M_3M_7$, $ M_7^2$, $ M_4\phi_1^2$, $ \phi_1q_2\tilde{q}_2$, $ M_4M_5$, $ M_2M_6$, $ M_3\phi_1^2$, $ M_7\phi_1^2$, $ \phi_1\tilde{q}_1^2$, $ M_2M_4$, $ M_3M_5$, $ M_5M_7$, $ \phi_1^4$, $ M_2M_3$, $ M_2M_7$, $ M_5\phi_1^2$, $ M_5^2$, $ M_2\phi_1^2$, $ M_2M_5$, $ M_2^2$ | . | -2 | t^2.2 + t^2.34 + 2*t^2.49 + t^2.63 + t^2.77 + t^2.91 + t^3.66 + t^3.94 + t^4.26 + 2*t^4.4 + 2*t^4.54 + 3*t^4.69 + 3*t^4.83 + 5*t^4.97 + 4*t^5.11 + t^5.15 + 3*t^5.25 + 2*t^5.4 + 2*t^5.54 + t^5.68 + t^5.82 - 2*t^6. + t^6.14 + t^6.28 + 2*t^6.43 + t^6.46 + t^6.57 + 2*t^6.6 + 3*t^6.75 + t^6.85 + 5*t^6.89 + 5*t^7.03 + 7*t^7.17 + 7*t^7.31 + t^7.35 + 9*t^7.46 + t^7.49 + 8*t^7.6 + t^7.63 + 7*t^7.74 + 7*t^7.88 - t^7.92 + 5*t^8.02 - t^8.06 + 4*t^8.16 - 4*t^8.2 + 3*t^8.31 - 4*t^8.34 + 2*t^8.45 - 5*t^8.49 + t^8.59 - 2*t^8.63 + t^8.66 + t^8.73 - 2*t^8.77 + 3*t^8.81 + 2*t^8.95 - t^4.31/y - t^6.51/y - t^6.66/y - t^6.8/y - t^6.94/y - t^7.08/y - t^7.22/y + t^7.4/y + (2*t^7.54)/y + (3*t^7.69)/y + (4*t^7.83)/y + (4*t^7.97)/y + (5*t^8.11)/y + (3*t^8.25)/y + (3*t^8.4)/y + t^8.54/y + t^8.68/y - t^8.72/y - t^4.31*y - t^6.51*y - t^6.66*y - t^6.8*y - t^6.94*y - t^7.08*y - t^7.22*y + t^7.4*y + 2*t^7.54*y + 3*t^7.69*y + 4*t^7.83*y + 4*t^7.97*y + 5*t^8.11*y + 3*t^8.25*y + 3*t^8.4*y + t^8.54*y + t^8.68*y - t^8.72*y | g1^7*t^2.2 + g1^2*t^2.34 + (2*t^2.49)/g1^3 + t^2.63/g1^8 + t^2.77/g1^13 + t^2.91/g1^18 + t^3.66/g1^2 + t^3.94/g1^12 + g1^19*t^4.26 + 2*g1^14*t^4.4 + 2*g1^9*t^4.54 + 3*g1^4*t^4.69 + (3*t^4.83)/g1 + (5*t^4.97)/g1^6 + (4*t^5.11)/g1^11 + g1^30*t^5.15 + (3*t^5.25)/g1^16 + (2*t^5.4)/g1^21 + (2*t^5.54)/g1^26 + t^5.68/g1^31 + t^5.82/g1^36 - 2*t^6. + t^6.14/g1^5 + t^6.28/g1^10 + (2*t^6.43)/g1^15 + g1^26*t^6.46 + t^6.57/g1^20 + 2*g1^21*t^6.6 + 3*g1^16*t^6.75 + t^6.85/g1^30 + 5*g1^11*t^6.89 + 5*g1^6*t^7.03 + 7*g1*t^7.17 + (7*t^7.31)/g1^4 + g1^37*t^7.35 + (9*t^7.46)/g1^9 + g1^32*t^7.49 + (8*t^7.6)/g1^14 + g1^27*t^7.63 + (7*t^7.74)/g1^19 + (7*t^7.88)/g1^24 - g1^17*t^7.92 + (5*t^8.02)/g1^29 - g1^12*t^8.06 + (4*t^8.16)/g1^34 - 4*g1^7*t^8.2 + (3*t^8.31)/g1^39 - 4*g1^2*t^8.34 + (2*t^8.45)/g1^44 - (5*t^8.49)/g1^3 + t^8.59/g1^49 - (2*t^8.63)/g1^8 + g1^33*t^8.66 + t^8.73/g1^54 - (2*t^8.77)/g1^13 + 3*g1^28*t^8.81 + 2*g1^23*t^8.95 - t^4.31/(g1^4*y) - (g1^3*t^6.51)/y - t^6.66/(g1^2*y) - t^6.8/(g1^7*y) - t^6.94/(g1^12*y) - t^7.08/(g1^17*y) - t^7.22/(g1^22*y) + (g1^14*t^7.4)/y + (2*g1^9*t^7.54)/y + (3*g1^4*t^7.69)/y + (4*t^7.83)/(g1*y) + (4*t^7.97)/(g1^6*y) + (5*t^8.11)/(g1^11*y) + (3*t^8.25)/(g1^16*y) + (3*t^8.4)/(g1^21*y) + t^8.54/(g1^26*y) + t^8.68/(g1^31*y) - (g1^10*t^8.72)/y - (t^4.31*y)/g1^4 - g1^3*t^6.51*y - (t^6.66*y)/g1^2 - (t^6.8*y)/g1^7 - (t^6.94*y)/g1^12 - (t^7.08*y)/g1^17 - (t^7.22*y)/g1^22 + g1^14*t^7.4*y + 2*g1^9*t^7.54*y + 3*g1^4*t^7.69*y + (4*t^7.83*y)/g1 + (4*t^7.97*y)/g1^6 + (5*t^8.11*y)/g1^11 + (3*t^8.25*y)/g1^16 + (3*t^8.4*y)/g1^21 + (t^8.54*y)/g1^26 + (t^8.68*y)/g1^31 - g1^10*t^8.72*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 |
|---|---|---|---|---|---|---|---|---|---|
| 50984 | 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$ + $ M_5q_2\tilde{q}_1$ + $ \phi_1\tilde{q}_2^2$ + $ M_4\phi_1q_1^2$ + $ M_6\phi_1q_1q_2$ | 0.6866 | 0.8604 | 0.798 | [X:[], M:[1.1704, 0.9776, 0.8296, 0.7803, 0.9283, 0.7309], q:[0.3901, 0.4395], qb:[0.6323, 0.7803], phi:[0.4395]] | t^2.19 + t^2.34 + t^2.49 + t^2.64 + t^2.78 + t^2.93 + t^3.51 + t^3.66 + t^3.96 + t^4.24 + 2*t^4.39 + 2*t^4.53 + 2*t^4.68 + 2*t^4.83 + 3*t^4.98 + t^5.11 + 3*t^5.13 + 2*t^5.27 + t^5.42 + 2*t^5.57 + t^5.7 + t^5.72 + t^5.85 + t^5.87 - t^6. - t^4.32/y - t^4.32*y | detail |