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 |
|---|---|---|---|---|---|---|---|---|---|
| 5899 | SU2adj1nf2 | $M_1q_1q_2$ + $ M_2\phi_1^2$ + $ M_3\tilde{q}_1\tilde{q}_2$ + $ M_4q_1\tilde{q}_1$ + $ M_5q_2\tilde{q}_2$ + $ M_6q_2\tilde{q}_1$ + $ M_4M_6$ + $ M_1^2$ + $ M_5M_7$ + $ \phi_1q_2^2$ + $ M_8\phi_1q_1^2$ + $ M_9\phi_1q_1\tilde{q}_2$ | 0.6061 | 0.7767 | 0.7803 | [X:[], M:[1.0, 1.0164, 0.9673, 1.2541, 0.7132, 0.7459, 1.2868, 1.0164, 0.7295], q:[0.2459, 0.7541], qb:[0.5, 0.5327], phi:[0.4918]] | [X:[], M:[[0], [4], [-8], [1], [-9], [-1], [9], [4], [-5]], q:[[-1], [1]], qb:[[0], [8]], phi:[[-2]]] | 1 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| $M_9$, $ M_6$, $ q_1\tilde{q}_2$, $ M_3$, $ M_1$, $ M_2$, $ M_8$, $ \phi_1q_1\tilde{q}_1$, $ M_4$, $ M_7$, $ M_9^2$, $ M_6M_9$, $ M_6^2$, $ \phi_1q_1q_2$, $ \phi_1\tilde{q}_1^2$, $ M_9q_1\tilde{q}_2$, $ M_6q_1\tilde{q}_2$, $ \phi_1\tilde{q}_1\tilde{q}_2$, $ \phi_1\tilde{q}_2^2$, $ q_1^2\tilde{q}_2^2$, $ M_3M_9$, $ M_1M_9$, $ M_1M_6$, $ M_2M_9$, $ M_8M_9$, $ \phi_1q_2\tilde{q}_1$, $ M_2M_6$, $ M_6M_8$, $ \phi_1q_2\tilde{q}_2$, $ M_2q_1\tilde{q}_2$, $ M_8q_1\tilde{q}_2$, $ M_3^2$, $ M_1M_3$, $ M_9\phi_1q_1\tilde{q}_1$, $ M_2M_3$, $ M_3M_8$, $ M_4M_9$, $ M_6\phi_1q_1\tilde{q}_1$ | . | -2 | t^2.19 + t^2.24 + t^2.34 + t^2.9 + t^3. + 2*t^3.05 + t^3.71 + t^3.76 + t^3.86 + t^4.38 + t^4.43 + 2*t^4.48 + t^4.52 + 2*t^4.57 + 2*t^4.67 + t^5.09 + t^5.19 + 3*t^5.24 + 2*t^5.29 + t^5.34 + 2*t^5.38 + t^5.8 + t^5.9 + 3*t^5.95 - 2*t^6. + 3*t^6.05 + 3*t^6.1 + t^6.2 + t^6.57 + t^6.62 + 2*t^6.66 + t^6.71 + 3*t^6.76 + 2*t^6.81 + t^6.86 + 4*t^6.91 + 2*t^7.01 + t^7.28 + t^7.38 + 3*t^7.43 + 2*t^7.48 + 2*t^7.52 + 3*t^7.57 + 3*t^7.62 + t^7.67 + 4*t^7.72 + t^7.99 + t^8.09 + 2*t^8.14 - t^8.19 + 3*t^8.29 + 2*t^8.38 + 4*t^8.43 + 2*t^8.53 + t^8.71 + t^8.75 + 2*t^8.8 + 3*t^8.85 - 2*t^8.9 + 3*t^8.95 - t^4.48/y - t^6.66/y - t^7.38/y + (2*t^7.43)/y + (2*t^7.57)/y + t^8.09/y + t^8.14/y + t^8.19/y + (4*t^8.24)/y + (3*t^8.29)/y + t^8.34/y + (2*t^8.38)/y - t^8.85/y + (2*t^8.9)/y + (4*t^8.95)/y - t^4.48*y - t^6.66*y - t^7.38*y + 2*t^7.43*y + 2*t^7.57*y + t^8.09*y + t^8.14*y + t^8.19*y + 4*t^8.24*y + 3*t^8.29*y + t^8.34*y + 2*t^8.38*y - t^8.85*y + 2*t^8.9*y + 4*t^8.95*y | t^2.19/g1^5 + t^2.24/g1 + g1^7*t^2.34 + t^2.9/g1^8 + t^3. + 2*g1^4*t^3.05 + t^3.71/g1^3 + g1*t^3.76 + g1^9*t^3.86 + t^4.38/g1^10 + t^4.43/g1^6 + (2*t^4.48)/g1^2 + g1^2*t^4.52 + 2*g1^6*t^4.57 + 2*g1^14*t^4.67 + t^5.09/g1^13 + t^5.19/g1^5 + (3*t^5.24)/g1 + 2*g1^3*t^5.29 + g1^7*t^5.34 + 2*g1^11*t^5.38 + t^5.8/g1^16 + t^5.9/g1^8 + (3*t^5.95)/g1^4 - 2*t^6. + 3*g1^4*t^6.05 + 3*g1^8*t^6.1 + g1^16*t^6.2 + t^6.57/g1^15 + t^6.62/g1^11 + (2*t^6.66)/g1^7 + t^6.71/g1^3 + 3*g1*t^6.76 + 2*g1^5*t^6.81 + g1^9*t^6.86 + 4*g1^13*t^6.91 + 2*g1^21*t^7.01 + t^7.28/g1^18 + t^7.38/g1^10 + (3*t^7.43)/g1^6 + (2*t^7.48)/g1^2 + 2*g1^2*t^7.52 + 3*g1^6*t^7.57 + 3*g1^10*t^7.62 + g1^14*t^7.67 + 4*g1^18*t^7.72 + t^7.99/g1^21 + t^8.09/g1^13 + (2*t^8.14)/g1^9 - t^8.19/g1^5 + 3*g1^3*t^8.29 + 2*g1^11*t^8.38 + 4*g1^15*t^8.43 + 2*g1^23*t^8.53 + t^8.71/g1^24 + t^8.75/g1^20 + (2*t^8.8)/g1^16 + (3*t^8.85)/g1^12 - (2*t^8.9)/g1^8 + (3*t^8.95)/g1^4 - t^4.48/(g1^2*y) - t^6.66/(g1^7*y) - t^7.38/(g1^10*y) + (2*t^7.43)/(g1^6*y) + (2*g1^6*t^7.57)/y + t^8.09/(g1^13*y) + t^8.14/(g1^9*y) + t^8.19/(g1^5*y) + (4*t^8.24)/(g1*y) + (3*g1^3*t^8.29)/y + (g1^7*t^8.34)/y + (2*g1^11*t^8.38)/y - t^8.85/(g1^12*y) + (2*t^8.9)/(g1^8*y) + (4*t^8.95)/(g1^4*y) - (t^4.48*y)/g1^2 - (t^6.66*y)/g1^7 - (t^7.38*y)/g1^10 + (2*t^7.43*y)/g1^6 + 2*g1^6*t^7.57*y + (t^8.09*y)/g1^13 + (t^8.14*y)/g1^9 + (t^8.19*y)/g1^5 + (4*t^8.24*y)/g1 + 3*g1^3*t^8.29*y + g1^7*t^8.34*y + 2*g1^11*t^8.38*y - (t^8.85*y)/g1^12 + (2*t^8.9*y)/g1^8 + (4*t^8.95*y)/g1^4 |
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 |
|---|---|---|---|---|---|---|---|---|---|
| 4401 | SU2adj1nf2 | $M_1q_1q_2$ + $ M_2\phi_1^2$ + $ M_3\tilde{q}_1\tilde{q}_2$ + $ M_4q_1\tilde{q}_1$ + $ M_5q_2\tilde{q}_2$ + $ M_6q_2\tilde{q}_1$ + $ M_4M_6$ + $ M_1^2$ + $ M_5M_7$ + $ \phi_1q_2^2$ + $ M_8\phi_1q_1^2$ | 0.5864 | 0.7409 | 0.7914 | [X:[], M:[1.0, 1.0109, 0.9781, 1.2527, 0.7254, 0.7473, 1.2746, 1.0109], q:[0.2473, 0.7527], qb:[0.5, 0.5219], phi:[0.4945]] | t^2.24 + t^2.31 + t^2.93 + t^3. + 2*t^3.03 + t^3.73 + t^3.76 + t^3.79 + t^3.82 + 2*t^4.48 + 2*t^4.55 + 2*t^4.61 + t^5.24 + 2*t^5.27 + t^5.31 + 2*t^5.34 + t^5.87 + 2*t^5.97 - 2*t^6. - t^4.48/y - t^4.48*y | detail |