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 |
|---|---|---|---|---|---|---|---|---|---|
| 56085 | 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}_1\tilde{q}_2$ + $ M_6\phi_1q_1^2$ + $ M_2\phi_1q_2^2$ + $ M_7\phi_1q_1q_2$ | 0.6915 | 0.8877 | 0.779 | [X:[], M:[1.1442, 0.7162, 0.8558, 0.8093, 0.6697, 0.8093, 0.7628], q:[0.4047, 0.4512], qb:[0.8791, 0.7395], phi:[0.3814]] | [X:[], M:[[12], [18], [-12], [-2], [28], [-2], [8]], q:[[-1], [-11]], qb:[[-17], [13]], phi:[[4]]] | 1 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| $M_5$, $ M_2$, $ M_7$, $ \phi_1^2$, $ M_4$, $ M_6$, $ M_3$, $ M_1$, $ \phi_1q_2^2$, $ M_5^2$, $ M_2M_5$, $ M_2^2$, $ M_5M_7$, $ M_5\phi_1^2$, $ M_4M_5$, $ M_5M_6$, $ M_2M_7$, $ M_2\phi_1^2$, $ M_2M_4$, $ M_3M_5$, $ M_2M_6$, $ M_7^2$, $ M_7\phi_1^2$, $ \phi_1^4$, $ \phi_1q_1\tilde{q}_2$, $ M_2M_3$, $ M_4M_7$, $ M_6M_7$, $ M_4\phi_1^2$, $ M_6\phi_1^2$, $ \phi_1q_2\tilde{q}_2$, $ M_4^2$, $ M_4M_6$, $ M_6^2$, $ M_3M_7$, $ M_3\phi_1^2$, $ \tilde{q}_1\tilde{q}_2$, $ M_3M_4$, $ M_3M_6$, $ \phi_1q_1\tilde{q}_1$, $ M_3^2$, $ \phi_1q_2\tilde{q}_1$, $ M_1M_5$, $ M_1M_2$, $ \phi_1\tilde{q}_2^2$, $ M_1M_7$, $ M_1\phi_1^2$, $ M_1M_4$, $ M_1M_6$, $ M_5\phi_1q_2^2$ | . | -1 | t^2.01 + t^2.15 + 2*t^2.29 + 2*t^2.43 + t^2.57 + t^3.43 + t^3.85 + t^4.02 + t^4.16 + 3*t^4.3 + 4*t^4.44 + 6*t^4.58 + 5*t^4.72 + 6*t^4.86 + 2*t^5. + t^5.14 + t^5.44 + t^5.58 + t^5.72 + t^5.86 - t^6. + t^6.03 + t^6.17 + t^6.28 + 3*t^6.31 + t^6.42 + 5*t^6.45 + 8*t^6.59 + 10*t^6.73 + 15*t^6.86 + 12*t^7. + 11*t^7.14 + 8*t^7.28 + 2*t^7.42 + t^7.45 + t^7.59 + t^7.7 + 2*t^7.73 + 2*t^7.87 + t^8.04 - 3*t^8.15 + t^8.18 - 4*t^8.29 + 3*t^8.32 - 7*t^8.43 + 5*t^8.46 - 5*t^8.57 + 9*t^8.59 + 12*t^8.73 + 20*t^8.87 + t^8.99 - t^4.14/y - t^6.15/y - t^6.29/y - (2*t^6.43)/y - (2*t^6.57)/y + t^7.16/y + (2*t^7.3)/y + (4*t^7.44)/y + (4*t^7.58)/y + (7*t^7.72)/y + (5*t^7.86)/y + (3*t^8.)/y + t^8.14/y - t^8.16/y - t^8.3/y - (2*t^8.44)/y - (3*t^8.58)/y - (3*t^8.72)/y - t^8.86/y - t^4.14*y - t^6.15*y - t^6.29*y - 2*t^6.43*y - 2*t^6.57*y + t^7.16*y + 2*t^7.3*y + 4*t^7.44*y + 4*t^7.58*y + 7*t^7.72*y + 5*t^7.86*y + 3*t^8.*y + t^8.14*y - t^8.16*y - t^8.3*y - 2*t^8.44*y - 3*t^8.58*y - 3*t^8.72*y - t^8.86*y | g1^28*t^2.01 + g1^18*t^2.15 + 2*g1^8*t^2.29 + (2*t^2.43)/g1^2 + t^2.57/g1^12 + g1^12*t^3.43 + t^3.85/g1^18 + g1^56*t^4.02 + g1^46*t^4.16 + 3*g1^36*t^4.3 + 4*g1^26*t^4.44 + 6*g1^16*t^4.58 + 5*g1^6*t^4.72 + (6*t^4.86)/g1^4 + (2*t^5.)/g1^14 + t^5.14/g1^24 + g1^40*t^5.44 + g1^30*t^5.58 + g1^20*t^5.72 + g1^10*t^5.86 - t^6. + g1^84*t^6.03 + g1^74*t^6.17 + t^6.28/g1^20 + 3*g1^64*t^6.31 + t^6.42/g1^30 + 5*g1^54*t^6.45 + 8*g1^44*t^6.59 + 10*g1^34*t^6.73 + 15*g1^24*t^6.86 + 12*g1^14*t^7. + 11*g1^4*t^7.14 + (8*t^7.28)/g1^6 + (2*t^7.42)/g1^16 + g1^68*t^7.45 + g1^58*t^7.59 + t^7.7/g1^36 + 2*g1^48*t^7.73 + 2*g1^38*t^7.87 + g1^112*t^8.04 - 3*g1^18*t^8.15 + g1^102*t^8.18 - 4*g1^8*t^8.29 + 3*g1^92*t^8.32 - (7*t^8.43)/g1^2 + 5*g1^82*t^8.46 - (5*t^8.57)/g1^12 + 9*g1^72*t^8.59 + 12*g1^62*t^8.73 + 20*g1^52*t^8.87 + t^8.99/g1^42 - (g1^4*t^4.14)/y - (g1^32*t^6.15)/y - (g1^22*t^6.29)/y - (2*g1^12*t^6.43)/y - (2*g1^2*t^6.57)/y + (g1^46*t^7.16)/y + (2*g1^36*t^7.3)/y + (4*g1^26*t^7.44)/y + (4*g1^16*t^7.58)/y + (7*g1^6*t^7.72)/y + (5*t^7.86)/(g1^4*y) + (3*t^8.)/(g1^14*y) + t^8.14/(g1^24*y) - (g1^60*t^8.16)/y - (g1^50*t^8.3)/y - (2*g1^40*t^8.44)/y - (3*g1^30*t^8.58)/y - (3*g1^20*t^8.72)/y - (g1^10*t^8.86)/y - g1^4*t^4.14*y - g1^32*t^6.15*y - g1^22*t^6.29*y - 2*g1^12*t^6.43*y - 2*g1^2*t^6.57*y + g1^46*t^7.16*y + 2*g1^36*t^7.3*y + 4*g1^26*t^7.44*y + 4*g1^16*t^7.58*y + 7*g1^6*t^7.72*y + (5*t^7.86*y)/g1^4 + (3*t^8.*y)/g1^14 + (t^8.14*y)/g1^24 - g1^60*t^8.16*y - g1^50*t^8.3*y - 2*g1^40*t^8.44*y - 3*g1^30*t^8.58*y - 3*g1^20*t^8.72*y - g1^10*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 |
|---|---|---|---|---|---|---|---|---|---|
| 50867 | 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}_1\tilde{q}_2$ + $ M_6\phi_1q_1^2$ + $ M_2\phi_1q_2^2$ | 0.6731 | 0.854 | 0.7881 | [X:[], M:[1.1481, 0.7221, 0.8519, 0.8087, 0.6789, 0.8087], q:[0.4043, 0.4476], qb:[0.8736, 0.7438], phi:[0.3827]] | t^2.04 + t^2.17 + t^2.3 + 2*t^2.43 + t^2.56 + t^3.44 + t^3.7 + t^3.83 + t^4.07 + t^4.2 + 2*t^4.33 + 3*t^4.46 + 4*t^4.59 + 3*t^4.72 + 5*t^4.85 + 2*t^4.98 + t^5.11 + t^5.48 + t^5.61 + t^5.74 + 2*t^5.87 - t^4.15/y - t^4.15*y | detail |