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 |
|---|---|---|---|---|---|---|---|---|---|
| 1941 | SU2adj1nf2 | $M_1q_1q_2$ + $ M_2\tilde{q}_1\tilde{q}_2$ + $ M_3q_1\tilde{q}_1$ + $ M_4q_2\tilde{q}_2$ + $ M_1M_3$ + $ M_2\phi_1^2$ + $ M_2M_5$ + $ \phi_1\tilde{q}_2^2$ | 0.5568 | 0.7209 | 0.7723 | [X:[], M:[0.8489, 1.0504, 1.1511, 0.7481, 0.9496], q:[0.6618, 0.4893], qb:[0.187, 0.7626], phi:[0.4748]] | [X:[], M:[[-12], [4], [12], [-20], [-4]], q:[[-7], [19]], qb:[[-5], [1]], phi:[[-2]]] | 1 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| $q_2\tilde{q}_1$, $ M_4$, $ M_1$, $ \phi_1\tilde{q}_1^2$, $ M_5$, $ \phi_1^2$, $ M_3$, $ \phi_1q_2\tilde{q}_1$, $ \phi_1q_1\tilde{q}_1$, $ q_2^2\tilde{q}_1^2$, $ M_4q_2\tilde{q}_1$, $ q_1\tilde{q}_2$, $ \phi_1\tilde{q}_1\tilde{q}_2$, $ \phi_1q_2^2$, $ M_4^2$, $ \phi_1q_2\tilde{q}_1^3$, $ M_1M_4$, $ M_4\phi_1\tilde{q}_1^2$, $ \phi_1q_1q_2$, $ M_5q_2\tilde{q}_1$, $ \phi_1^2q_2\tilde{q}_1$, $ M_1^2$, $ M_4M_5$, $ M_4\phi_1^2$, $ M_1\phi_1\tilde{q}_1^2$, $ \phi_1^2\tilde{q}_1^4$, $ M_1M_5$, $ M_1\phi_1^2$, $ \phi_1q_1^2$, $ M_5\phi_1\tilde{q}_1^2$, $ \phi_1^3\tilde{q}_1^2$, $ M_3q_2\tilde{q}_1$, $ \phi_1q_2^2\tilde{q}_1^2$, $ M_3M_4$, $ M_5^2$, $ M_5\phi_1^2$, $ \phi_1^4$, $ M_4\phi_1q_2\tilde{q}_1$, $ \phi_1q_1\tilde{q}_2$ | $M_3\phi_1\tilde{q}_1^2$, $ \phi_1^2q_2\tilde{q}_1^3$ | 0 | t^2.03 + t^2.24 + 2*t^2.55 + 2*t^2.85 + 2*t^3.45 + t^3.97 + t^4.06 + 2*t^4.27 + t^4.36 + t^4.49 + t^4.58 + 2*t^4.79 + 3*t^4.88 + 4*t^5.09 + 5*t^5.4 + t^5.48 + 3*t^5.7 + t^6.09 + t^6.22 + 3*t^6.3 + t^6.39 + 2*t^6.52 + t^6.73 + 3*t^6.82 + 4*t^6.91 + 2*t^7.04 + 3*t^7.12 + t^7.21 + 4*t^7.34 + t^7.42 + 7*t^7.64 + 3*t^7.73 + 2*t^7.81 + 8*t^7.94 - 3*t^8.03 + t^8.12 + 4*t^8.24 + 2*t^8.33 + t^8.42 + t^8.46 - t^8.55 + t^8.72 + 2*t^8.76 - 3*t^8.85 + 2*t^8.94 + t^8.98 - t^4.42/y - t^6.67/y + (3*t^7.58)/y + (2*t^7.79)/y + (2*t^7.88)/y + (3*t^8.09)/y + t^8.18/y + (4*t^8.4)/y + (2*t^8.48)/y + (3*t^8.7)/y - t^8.91/y - t^4.42*y - t^6.67*y + 3*t^7.58*y + 2*t^7.79*y + 2*t^7.88*y + 3*t^8.09*y + t^8.18*y + 4*t^8.4*y + 2*t^8.48*y + 3*t^8.7*y - t^8.91*y | g1^14*t^2.03 + t^2.24/g1^20 + (2*t^2.55)/g1^12 + (2*t^2.85)/g1^4 + 2*g1^12*t^3.45 + t^3.97/g1^14 + g1^28*t^4.06 + (2*t^4.27)/g1^6 + g1^36*t^4.36 + t^4.49/g1^40 + g1^2*t^4.58 + (2*t^4.79)/g1^32 + 3*g1^10*t^4.88 + (4*t^5.09)/g1^24 + (5*t^5.4)/g1^16 + g1^26*t^5.48 + (3*t^5.7)/g1^8 + g1^42*t^6.09 + t^6.22/g1^34 + 3*g1^8*t^6.3 + g1^50*t^6.39 + (2*t^6.52)/g1^26 + t^6.73/g1^60 + (3*t^6.82)/g1^18 + 4*g1^24*t^6.91 + (2*t^7.04)/g1^52 + (3*t^7.12)/g1^10 + g1^32*t^7.21 + (4*t^7.34)/g1^44 + t^7.42/g1^2 + (7*t^7.64)/g1^36 + 3*g1^6*t^7.73 + 2*g1^48*t^7.81 + (8*t^7.94)/g1^28 - 3*g1^14*t^8.03 + g1^56*t^8.12 + (4*t^8.24)/g1^20 + 2*g1^22*t^8.33 + g1^64*t^8.42 + t^8.46/g1^54 - t^8.55/g1^12 + g1^72*t^8.72 + (2*t^8.76)/g1^46 - (3*t^8.85)/g1^4 + 2*g1^38*t^8.94 + t^8.98/g1^80 - t^4.42/(g1^2*y) - t^6.67/(g1^22*y) + (3*g1^2*t^7.58)/y + (2*t^7.79)/(g1^32*y) + (2*g1^10*t^7.88)/y + (3*t^8.09)/(g1^24*y) + (g1^18*t^8.18)/y + (4*t^8.4)/(g1^16*y) + (2*g1^26*t^8.48)/y + (3*t^8.7)/(g1^8*y) - t^8.91/(g1^42*y) - (t^4.42*y)/g1^2 - (t^6.67*y)/g1^22 + 3*g1^2*t^7.58*y + (2*t^7.79*y)/g1^32 + 2*g1^10*t^7.88*y + (3*t^8.09*y)/g1^24 + g1^18*t^8.18*y + (4*t^8.4*y)/g1^16 + 2*g1^26*t^8.48*y + (3*t^8.7*y)/g1^8 - (t^8.91*y)/g1^42 |
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 |
|---|---|---|---|---|---|---|---|---|---|
| 584 | SU2adj1nf2 | $M_1q_1q_2$ + $ M_2\tilde{q}_1\tilde{q}_2$ + $ M_3q_1\tilde{q}_1$ + $ M_4q_2\tilde{q}_2$ + $ M_1M_3$ + $ M_2\phi_1^2$ + $ M_2M_5$ | 0.6993 | 0.8588 | 0.8143 | [X:[], M:[0.9384, 1.0205, 1.0616, 0.8973, 0.9795], q:[0.488, 0.5736], qb:[0.4504, 0.5291], phi:[0.4897]] | t^2.69 + t^2.82 + 2*t^2.94 + t^3.05 + t^3.07 + t^3.18 + t^4.17 + t^4.28 + t^4.4 + t^4.41 + t^4.52 + t^4.54 + t^4.64 + t^4.65 + t^4.78 + t^4.91 + t^5.38 + t^5.51 + 2*t^5.63 + 2*t^5.75 + 3*t^5.88 + 2*t^5.99 - 3*t^6. - t^4.47/y - t^4.47*y | detail |