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 |
|---|---|---|---|---|---|---|---|---|---|
| 56416 | 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$ + $ \phi_1\tilde{q}_2^2$ + $ M_5\phi_1q_1^2$ + $ M_2\phi_1^2$ + $ M_6\phi_1q_1q_2$ + $ M_7\phi_1^2$ | 0.6908 | 0.8754 | 0.7891 | [X:[], M:[1.1629, 1.0697, 0.8371, 0.7909, 0.7439, 0.6977, 1.0697], q:[0.3955, 0.4416], qb:[0.5348, 0.7674], phi:[0.4652]] | [X:[], M:[[-5], [4], [5], [-12], [14], [-3], [4]], q:[[-6], [11]], qb:[[2], [1]], phi:[[-2]]] | 1 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| $M_6$, $ M_5$, $ M_4$, $ M_3$, $ q_2\tilde{q}_1$, $ M_2$, $ M_7$, $ M_1$, $ \tilde{q}_1\tilde{q}_2$, $ \phi_1q_2^2$, $ M_6^2$, $ \phi_1q_1\tilde{q}_1$, $ M_5M_6$, $ \phi_1q_2\tilde{q}_1$, $ M_5^2$, $ M_4M_6$, $ M_4M_5$, $ M_3M_6$, $ \phi_1\tilde{q}_1^2$, $ M_3M_5$, $ M_4^2$, $ M_3M_4$, $ \phi_1q_1\tilde{q}_2$, $ M_3^2$, $ M_6q_2\tilde{q}_1$, $ \phi_1q_2\tilde{q}_2$, $ M_5q_2\tilde{q}_1$, $ M_2M_6$, $ M_6M_7$, $ M_4q_2\tilde{q}_1$, $ \phi_1\tilde{q}_1\tilde{q}_2$, $ M_2M_5$, $ M_5M_7$, $ M_3q_2\tilde{q}_1$, $ M_2M_4$, $ M_1M_6$, $ M_4M_7$, $ M_2M_3$, $ M_1M_5$, $ M_3M_7$, $ q_2^2\tilde{q}_1^2$ | $M_6\tilde{q}_1\tilde{q}_2$ | -1 | t^2.09 + t^2.23 + t^2.37 + t^2.51 + t^2.93 + 2*t^3.21 + t^3.49 + t^3.91 + t^4.05 + 2*t^4.19 + 2*t^4.32 + t^4.46 + t^4.47 + 3*t^4.6 + t^4.74 + t^4.75 + t^4.88 + 2*t^5.02 + t^5.16 + 3*t^5.3 + 3*t^5.44 + 2*t^5.58 + 2*t^5.72 + t^5.86 - t^6. + 3*t^6.14 + 2*t^6.28 + 6*t^6.42 + 5*t^6.56 + 5*t^6.7 + 5*t^6.84 + 2*t^6.97 + t^6.98 + 4*t^7.12 + 4*t^7.25 + t^7.39 + 3*t^7.4 + 6*t^7.53 + 3*t^7.67 + 2*t^7.68 + 3*t^7.81 + 5*t^7.95 + 2*t^8.23 + 3*t^8.37 + 4*t^8.51 + 9*t^8.65 + 9*t^8.79 + 7*t^8.93 - t^4.4/y - t^6.49/y - t^6.63/y - t^6.77/y + t^7.19/y + t^7.32/y + t^7.47/y + t^7.6/y + t^7.74/y + t^7.88/y + (2*t^8.02)/y + (2*t^8.16)/y + (4*t^8.3)/y + (3*t^8.44)/y + (2*t^8.58)/y + (2*t^8.72)/y - t^8.86/y - t^4.4*y - t^6.49*y - t^6.63*y - t^6.77*y + t^7.19*y + t^7.32*y + t^7.47*y + t^7.6*y + t^7.74*y + t^7.88*y + 2*t^8.02*y + 2*t^8.16*y + 4*t^8.3*y + 3*t^8.44*y + 2*t^8.58*y + 2*t^8.72*y - t^8.86*y | t^2.09/g1^3 + g1^14*t^2.23 + t^2.37/g1^12 + g1^5*t^2.51 + g1^13*t^2.93 + 2*g1^4*t^3.21 + t^3.49/g1^5 + g1^3*t^3.91 + g1^20*t^4.05 + (2*t^4.19)/g1^6 + 2*g1^11*t^4.32 + g1^28*t^4.46 + t^4.47/g1^15 + 3*g1^2*t^4.6 + g1^19*t^4.74 + t^4.75/g1^24 + t^4.88/g1^7 + 2*g1^10*t^5.02 + g1^27*t^5.16 + 3*g1*t^5.3 + 3*g1^18*t^5.44 + (2*t^5.58)/g1^8 + 2*g1^9*t^5.72 + g1^26*t^5.86 - t^6. + 3*g1^17*t^6.14 + t^6.28/g1^9 + g1^34*t^6.28 + 6*g1^8*t^6.42 + (2*t^6.56)/g1^18 + 3*g1^25*t^6.56 + (4*t^6.7)/g1 + g1^42*t^6.7 + t^6.84/g1^27 + 4*g1^16*t^6.84 + 2*g1^33*t^6.97 + t^6.98/g1^10 + t^7.12/g1^36 + 3*g1^7*t^7.12 + 4*g1^24*t^7.25 + g1^41*t^7.39 + (3*t^7.4)/g1^2 + 6*g1^15*t^7.53 + 3*g1^32*t^7.67 + (2*t^7.68)/g1^11 + 3*g1^6*t^7.81 + t^7.95/g1^20 + 4*g1^23*t^7.95 - (2*t^8.09)/g1^3 + 2*g1^40*t^8.09 + 2*g1^14*t^8.23 - (2*t^8.37)/g1^12 + 5*g1^31*t^8.37 + 3*g1^5*t^8.51 + g1^48*t^8.51 + t^8.65/g1^21 + 8*g1^22*t^8.65 + (5*t^8.79)/g1^4 + 4*g1^39*t^8.79 + (2*t^8.93)/g1^30 + 4*g1^13*t^8.93 + g1^56*t^8.93 - t^4.4/(g1^2*y) - t^6.49/(g1^5*y) - (g1^12*t^6.63)/y - t^6.77/(g1^14*y) + t^7.19/(g1^6*y) + (g1^11*t^7.32)/y + t^7.47/(g1^15*y) + (g1^2*t^7.6)/y + (g1^19*t^7.74)/y + t^7.88/(g1^7*y) + (2*g1^10*t^8.02)/y + t^8.16/(g1^16*y) + (g1^27*t^8.16)/y + (4*g1*t^8.3)/y + (3*g1^18*t^8.44)/y + (2*t^8.58)/(g1^8*y) + (2*g1^9*t^8.72)/y - (g1^26*t^8.86)/y - (t^4.4*y)/g1^2 - (t^6.49*y)/g1^5 - g1^12*t^6.63*y - (t^6.77*y)/g1^14 + (t^7.19*y)/g1^6 + g1^11*t^7.32*y + (t^7.47*y)/g1^15 + g1^2*t^7.6*y + g1^19*t^7.74*y + (t^7.88*y)/g1^7 + 2*g1^10*t^8.02*y + (t^8.16*y)/g1^16 + g1^27*t^8.16*y + 4*g1*t^8.3*y + 3*g1^18*t^8.44*y + (2*t^8.58*y)/g1^8 + 2*g1^9*t^8.72*y - g1^26*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 |
|---|---|---|---|---|---|---|---|---|---|
| 52344 | 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$ + $ \phi_1\tilde{q}_2^2$ + $ M_5\phi_1q_1^2$ + $ M_2\phi_1^2$ + $ M_6\phi_1q_1q_2$ | 0.6974 | 0.8857 | 0.7874 | [X:[], M:[1.159, 1.0728, 0.841, 0.7815, 0.7549, 0.6954], q:[0.3907, 0.4503], qb:[0.5364, 0.7682], phi:[0.4636]] | t^2.09 + t^2.26 + t^2.34 + t^2.52 + t^2.78 + t^2.96 + t^3.22 + t^3.48 + t^3.91 + t^4.09 + 2*t^4.17 + 2*t^4.35 + t^4.43 + t^4.53 + 3*t^4.61 + t^4.69 + t^4.79 + 2*t^4.87 + 3*t^5.05 + t^5.13 + t^5.22 + 3*t^5.3 + 2*t^5.48 + 2*t^5.56 + 2*t^5.74 + t^5.92 - t^4.39/y - t^4.39*y | detail |