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 |
|---|---|---|---|---|---|---|---|---|---|
| 55644 | SU2adj1nf2 | $M_1q_1q_2$ + $ M_2q_1\tilde{q}_1$ + $ M_3\tilde{q}_1\tilde{q}_2$ + $ M_4q_2\tilde{q}_2$ + $ M_1\phi_1^2$ + $ M_3M_4$ + $ M_4M_5$ + $ \phi_1\tilde{q}_1^2$ + $ M_6\phi_1q_2\tilde{q}_2$ | 0.6952 | 0.8862 | 0.7845 | [X:[], M:[1.0559, 0.7204, 0.8322, 1.1678, 0.8322, 0.6957], q:[0.5156, 0.4285], qb:[0.764, 0.4038], phi:[0.472]] | [X:[], M:[[4], [-20], [-12], [12], [-12], [14]], q:[[19], [-23]], qb:[[1], [11]], phi:[[-2]]] | 1 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| $M_6$, $ M_2$, $ M_3$, $ M_5$, $ q_1\tilde{q}_2$, $ \phi_1^2$, $ M_1$, $ q_2\tilde{q}_1$, $ \phi_1\tilde{q}_2^2$, $ \phi_1q_2^2$, $ M_6^2$, $ \phi_1q_1\tilde{q}_2$, $ M_2M_6$, $ \phi_1q_1q_2$, $ M_2^2$, $ \phi_1q_1^2$, $ M_3M_6$, $ M_5M_6$, $ M_2M_3$, $ M_2M_5$, $ M_6q_1\tilde{q}_2$, $ M_6\phi_1^2$, $ \phi_1\tilde{q}_1\tilde{q}_2$, $ M_3^2$, $ M_3M_5$, $ M_5^2$, $ M_2\phi_1^2$, $ \phi_1q_2\tilde{q}_1$, $ M_1M_6$, $ \phi_1q_1\tilde{q}_1$, $ M_3q_1\tilde{q}_2$, $ M_5q_1\tilde{q}_2$, $ M_1M_2$, $ M_3\phi_1^2$, $ M_5\phi_1^2$, $ q_1^2\tilde{q}_2^2$, $ \phi_1^2q_1\tilde{q}_2$, $ M_1M_3$, $ M_1M_5$, $ \phi_1^4$, $ M_6q_2\tilde{q}_1$, $ M_6\phi_1\tilde{q}_2^2$ | $M_2\phi_1\tilde{q}_2^2$ | -1 | t^2.09 + t^2.16 + 2*t^2.5 + t^2.76 + t^2.83 + t^3.17 + t^3.58 + t^3.84 + t^3.99 + 2*t^4.17 + 2*t^4.25 + t^4.32 + t^4.51 + 2*t^4.58 + 2*t^4.66 + t^4.85 + 2*t^4.92 + 4*t^4.99 + 3*t^5.25 + 3*t^5.33 + t^5.52 + t^5.59 + 3*t^5.66 + t^5.93 - t^6. + 2*t^6.07 + t^6.15 + t^6.26 + 4*t^6.34 + 2*t^6.41 + 3*t^6.48 + 2*t^6.6 + 4*t^6.67 + 4*t^6.75 + 3*t^6.82 + 2*t^6.93 + 4*t^7.01 + 3*t^7.08 + 4*t^7.15 + t^7.27 + 3*t^7.34 + 3*t^7.42 + 5*t^7.49 + t^7.56 + t^7.6 + t^7.68 + 5*t^7.75 + 5*t^7.83 + t^7.97 + 3*t^8.01 + 3*t^8.16 + t^8.24 + t^8.27 + t^8.31 + 3*t^8.35 + 2*t^8.42 + 4*t^8.57 + 3*t^8.64 + 3*t^8.68 + t^8.76 + 3*t^8.83 + 4*t^8.91 + 6*t^8.98 - t^4.42/y - t^6.5/y - t^6.58/y - t^6.91/y + t^7.25/y + (2*t^7.58)/y + (2*t^7.66)/y + t^7.85/y + (3*t^7.92)/y + (2*t^7.99)/y + (4*t^8.25)/y + (4*t^8.33)/y + (2*t^8.66)/y + (2*t^8.93)/y - t^4.42*y - t^6.5*y - t^6.58*y - t^6.91*y + t^7.25*y + 2*t^7.58*y + 2*t^7.66*y + t^7.85*y + 3*t^7.92*y + 2*t^7.99*y + 4*t^8.25*y + 4*t^8.33*y + 2*t^8.66*y + 2*t^8.93*y | g1^14*t^2.09 + t^2.16/g1^20 + (2*t^2.5)/g1^12 + g1^30*t^2.76 + t^2.83/g1^4 + g1^4*t^3.17 + t^3.58/g1^22 + g1^20*t^3.84 + t^3.99/g1^48 + 2*g1^28*t^4.17 + (2*t^4.25)/g1^6 + t^4.32/g1^40 + g1^36*t^4.51 + 2*g1^2*t^4.58 + (2*t^4.66)/g1^32 + g1^44*t^4.85 + 2*g1^10*t^4.92 + (4*t^4.99)/g1^24 + 3*g1^18*t^5.25 + (3*t^5.33)/g1^16 + g1^60*t^5.52 + g1^26*t^5.59 + (3*t^5.66)/g1^8 + g1^34*t^5.93 - t^6. + (2*t^6.07)/g1^34 + t^6.15/g1^68 + g1^42*t^6.26 + 4*g1^8*t^6.34 + (2*t^6.41)/g1^26 + (3*t^6.48)/g1^60 + 2*g1^50*t^6.6 + 4*g1^16*t^6.67 + (4*t^6.75)/g1^18 + (3*t^6.82)/g1^52 + 2*g1^58*t^6.93 + 4*g1^24*t^7.01 + (3*t^7.08)/g1^10 + (4*t^7.15)/g1^44 + g1^66*t^7.27 + 3*g1^32*t^7.34 + (3*t^7.42)/g1^2 + (5*t^7.49)/g1^36 + t^7.56/g1^70 + g1^74*t^7.6 + g1^40*t^7.68 + 5*g1^6*t^7.75 + (5*t^7.83)/g1^28 + t^7.97/g1^96 + 3*g1^48*t^8.01 + (3*t^8.16)/g1^20 + t^8.24/g1^54 + g1^90*t^8.27 + t^8.31/g1^88 + 3*g1^56*t^8.35 + 2*g1^22*t^8.42 + (4*t^8.57)/g1^46 + (3*t^8.64)/g1^80 + 3*g1^64*t^8.68 + g1^30*t^8.76 + (3*t^8.83)/g1^4 + (4*t^8.91)/g1^38 + (6*t^8.98)/g1^72 - t^4.42/(g1^2*y) - (g1^12*t^6.5)/y - t^6.58/(g1^22*y) - t^6.91/(g1^14*y) + t^7.25/(g1^6*y) + (2*g1^2*t^7.58)/y + (2*t^7.66)/(g1^32*y) + (g1^44*t^7.85)/y + (3*g1^10*t^7.92)/y + (2*t^7.99)/(g1^24*y) + (4*g1^18*t^8.25)/y + (4*t^8.33)/(g1^16*y) + (2*t^8.66)/(g1^8*y) + (2*g1^34*t^8.93)/y - (t^4.42*y)/g1^2 - g1^12*t^6.5*y - (t^6.58*y)/g1^22 - (t^6.91*y)/g1^14 + (t^7.25*y)/g1^6 + 2*g1^2*t^7.58*y + (2*t^7.66*y)/g1^32 + g1^44*t^7.85*y + 3*g1^10*t^7.92*y + (2*t^7.99*y)/g1^24 + 4*g1^18*t^8.25*y + (4*t^8.33*y)/g1^16 + (2*t^8.66*y)/g1^8 + 2*g1^34*t^8.93*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 |
|---|---|---|---|---|---|---|---|---|---|
| 47215 | SU2adj1nf2 | $M_1q_1q_2$ + $ M_2q_1\tilde{q}_1$ + $ M_3\tilde{q}_1\tilde{q}_2$ + $ M_4q_2\tilde{q}_2$ + $ M_1\phi_1^2$ + $ M_3M_4$ + $ M_4M_5$ + $ \phi_1\tilde{q}_1^2$ | 0.6746 | 0.8467 | 0.7967 | [X:[], M:[1.0563, 0.7183, 0.831, 1.169, 0.831], q:[0.5176, 0.426], qb:[0.7641, 0.4049], phi:[0.4718]] | t^2.15 + 2*t^2.49 + t^2.77 + t^2.83 + t^3.17 + t^3.57 + t^3.85 + t^3.91 + t^3.97 + t^4.18 + t^4.25 + t^4.31 + t^4.52 + 2*t^4.65 + t^4.92 + 4*t^4.99 + 2*t^5.26 + 3*t^5.32 + t^5.54 + t^5.6 + 2*t^5.66 - t^6. - t^4.42/y - t^4.42*y | detail |