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 |
|---|---|---|---|---|---|---|---|---|---|
| 46350 | SU2adj1nf2 | $M_1q_1q_2$ + $ M_2q_1\tilde{q}_1$ + $ \phi_1q_1^2$ + $ M_1\phi_1^2$ + $ M_2\phi_1q_2^2$ + $ M_1M_3$ + $ M_2M_4$ | 0.5923 | 0.7564 | 0.783 | [X:[], M:[0.9496, 0.8487, 1.0504, 1.1513], q:[0.7374, 0.313], qb:[0.4139, 0.4348], phi:[0.5252]] | [X:[], M:[[4], [12], [-4], [-12]], q:[[1], [-5]], qb:[[-13], [25]], phi:[[-2]]] | 1 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| $q_2\tilde{q}_1$, $ q_2\tilde{q}_2$, $ \tilde{q}_1\tilde{q}_2$, $ M_3$, $ \phi_1^2$, $ M_4$, $ \phi_1q_2^2$, $ q_1\tilde{q}_2$, $ \phi_1q_2\tilde{q}_1$, $ \phi_1q_2\tilde{q}_2$, $ \phi_1\tilde{q}_1^2$, $ \phi_1\tilde{q}_1\tilde{q}_2$, $ \phi_1\tilde{q}_2^2$, $ q_2^2\tilde{q}_1^2$, $ q_2^2\tilde{q}_1\tilde{q}_2$, $ q_2^2\tilde{q}_2^2$, $ \phi_1q_1q_2$, $ q_2\tilde{q}_1^2\tilde{q}_2$, $ q_2\tilde{q}_1\tilde{q}_2^2$, $ \phi_1q_1\tilde{q}_2$, $ \tilde{q}_1^2\tilde{q}_2^2$, $ M_3q_2\tilde{q}_1$, $ \phi_1^2q_2\tilde{q}_1$, $ M_3q_2\tilde{q}_2$, $ \phi_1^2q_2\tilde{q}_2$, $ M_4q_2\tilde{q}_1$, $ \phi_1q_2^3\tilde{q}_1$, $ M_4q_2\tilde{q}_2$, $ \phi_1q_2^3\tilde{q}_2$, $ M_3\tilde{q}_1\tilde{q}_2$, $ \phi_1^2\tilde{q}_1\tilde{q}_2$, $ q_1q_2\tilde{q}_2^2$ | $M_4\tilde{q}_1\tilde{q}_2$, $ 2\phi_1q_2^2\tilde{q}_1\tilde{q}_2$ | 0 | t^2.18 + t^2.24 + t^2.55 + 2*t^3.15 + 2*t^3.45 + t^3.52 + t^3.76 + t^3.82 + t^4.06 + t^4.12 + t^4.18 + t^4.36 + t^4.42 + t^4.49 + t^4.73 + t^4.79 + t^5.09 + 2*t^5.33 + 2*t^5.39 + t^5.63 + 3*t^5.7 + t^5.76 + t^6.06 + t^6.24 + 2*t^6.3 + t^6.37 + t^6.43 + t^6.54 + 4*t^6.61 + 2*t^6.67 + 2*t^6.73 + 3*t^6.91 + 2*t^6.97 + t^7.03 + 2*t^7.21 + 2*t^7.27 + 3*t^7.34 + 3*t^7.51 + t^7.58 + 4*t^7.64 + t^7.7 + 2*t^7.82 + t^7.88 + 2*t^7.94 + 2*t^8. + t^8.12 - t^8.18 + t^8.24 + 2*t^8.31 + t^8.37 + t^8.42 + t^8.48 + t^8.61 + t^8.67 + t^8.72 + 2*t^8.79 + 2*t^8.85 + 2*t^8.91 + 2*t^8.97 - t^4.58/y + (2*t^7.42)/y + t^7.79/y + (2*t^8.33)/y + (2*t^8.39)/y + (2*t^8.63)/y + (5*t^8.7)/y + t^8.76/y + t^8.94/y - t^4.58*y + 2*t^7.42*y + t^7.79*y + 2*t^8.33*y + 2*t^8.39*y + 2*t^8.63*y + 5*t^8.7*y + t^8.76*y + t^8.94*y | t^2.18/g1^18 + g1^20*t^2.24 + g1^12*t^2.55 + (2*t^3.15)/g1^4 + (2*t^3.45)/g1^12 + g1^26*t^3.52 + t^3.76/g1^20 + g1^18*t^3.82 + t^4.06/g1^28 + g1^10*t^4.12 + g1^48*t^4.18 + t^4.36/g1^36 + g1^2*t^4.42 + g1^40*t^4.49 + t^4.73/g1^6 + g1^32*t^4.79 + g1^24*t^5.09 + (2*t^5.33)/g1^22 + 2*g1^16*t^5.39 + t^5.63/g1^30 + 3*g1^8*t^5.7 + g1^46*t^5.76 + g1^38*t^6.06 + t^6.24/g1^46 + (2*t^6.3)/g1^8 + g1^30*t^6.37 + g1^68*t^6.43 + t^6.54/g1^54 + (4*t^6.61)/g1^16 + 2*g1^22*t^6.67 + 2*g1^60*t^6.73 + (3*t^6.91)/g1^24 + 2*g1^14*t^6.97 + g1^52*t^7.03 + (2*t^7.21)/g1^32 + 2*g1^6*t^7.27 + 3*g1^44*t^7.34 + (3*t^7.51)/g1^40 + t^7.58/g1^2 + 4*g1^36*t^7.64 + g1^74*t^7.7 + (2*t^7.82)/g1^48 + t^7.88/g1^10 + 2*g1^28*t^7.94 + 2*g1^66*t^8. + t^8.12/g1^56 - t^8.18/g1^18 + g1^20*t^8.24 + 2*g1^58*t^8.31 + g1^96*t^8.37 + t^8.42/g1^64 + t^8.48/g1^26 + g1^50*t^8.61 + g1^88*t^8.67 + t^8.72/g1^72 + (2*t^8.79)/g1^34 + 2*g1^4*t^8.85 + 2*g1^42*t^8.91 + 2*g1^80*t^8.97 - t^4.58/(g1^2*y) + (2*g1^2*t^7.42)/y + (g1^32*t^7.79)/y + (2*t^8.33)/(g1^22*y) + (2*g1^16*t^8.39)/y + (2*t^8.63)/(g1^30*y) + (5*g1^8*t^8.7)/y + (g1^46*t^8.76)/y + t^8.94/(g1^38*y) - (t^4.58*y)/g1^2 + 2*g1^2*t^7.42*y + g1^32*t^7.79*y + (2*t^8.33*y)/g1^22 + 2*g1^16*t^8.39*y + (2*t^8.63*y)/g1^30 + 5*g1^8*t^8.7*y + g1^46*t^8.76*y + (t^8.94*y)/g1^38 |
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 |
|---|---|---|---|---|---|---|---|---|
| 48111 | $M_1q_1q_2$ + $ M_2q_1\tilde{q}_1$ + $ \phi_1q_1^2$ + $ M_1\phi_1^2$ + $ M_2\phi_1q_2^2$ + $ M_1M_3$ + $ M_2M_4$ + $ M_5\tilde{q}_1\tilde{q}_2$ | 0.5793 | 0.7341 | 0.7892 | [X:[], M:[0.9519, 0.8556, 1.0481, 1.1444, 1.1444], q:[0.738, 0.3102], qb:[0.4064, 0.4492], phi:[0.5241]] | t^2.15 + t^2.28 + 2*t^3.14 + 3*t^3.43 + t^3.56 + t^3.72 + t^3.85 + t^4.01 + t^4.14 + t^4.27 + t^4.3 + t^4.43 + t^4.56 + 2*t^5.29 + 2*t^5.42 + 2*t^5.58 + 2*t^5.71 + t^5.84 - 2*t^6. - t^4.57/y - t^4.57*y | detail |
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 |
|---|---|---|---|---|---|---|---|---|---|
| 46189 | SU2adj1nf2 | $M_1q_1q_2$ + $ M_2q_1\tilde{q}_1$ + $ \phi_1q_1^2$ + $ M_1\phi_1^2$ + $ M_2\phi_1q_2^2$ + $ M_1M_3$ | 0.6057 | 0.7801 | 0.7765 | [X:[], M:[0.9474, 0.8422, 1.0526], q:[0.7368, 0.3158], qb:[0.421, 0.4212], phi:[0.5263]] | 2*t^2.21 + 2*t^2.53 + 2*t^3.16 + 2*t^3.47 + 2*t^3.79 + t^4.1 + 2*t^4.11 + 3*t^4.42 + 4*t^4.74 + 3*t^5.05 + 4*t^5.37 + 5*t^5.68 + 2*t^6. - t^4.58/y - t^4.58*y | detail |