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 |
|---|---|---|---|---|---|---|---|---|---|
| 46939 | 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_1M_5$ + $ M_2\phi_1^2$ + $ M_6\phi_1^2$ | 0.705 | 0.865 | 0.815 | [X:[], M:[1.0401, 1.0401, 0.8797, 0.8797, 0.9599, 1.0401], q:[0.4432, 0.5167], qb:[0.5167, 0.6036], phi:[0.4799]] | [X:[], M:[[2, 2], [2, 2], [-6, -6], [-6, -6], [-2, -2], [2, 2]], q:[[-8, -2], [6, 0]], qb:[[6, 0], [0, 6]], phi:[[-1, -1]]] | 2 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| $M_3$, $ M_4$, $ M_5$, $ q_2\tilde{q}_1$, $ M_2$, $ M_6$, $ q_1\tilde{q}_2$, $ \phi_1q_1^2$, $ \phi_1q_1q_2$, $ \phi_1q_1\tilde{q}_1$, $ \phi_1q_2^2$, $ \phi_1q_2\tilde{q}_1$, $ \phi_1\tilde{q}_1^2$, $ \phi_1q_1\tilde{q}_2$, $ \phi_1q_2\tilde{q}_2$, $ \phi_1\tilde{q}_1\tilde{q}_2$, $ \phi_1\tilde{q}_2^2$, $ M_3^2$, $ M_3M_4$, $ M_4^2$, $ M_3M_5$, $ M_4M_5$, $ M_2M_3$, $ M_2M_4$, $ M_5^2$, $ M_3M_6$, $ M_4M_6$, $ M_5q_2\tilde{q}_1$ | $M_2M_5$, $ M_5M_6$ | -4 | 2*t^2.64 + t^2.88 + t^3.1 + 2*t^3.12 + t^3.14 + t^4.1 + 2*t^4.32 + 3*t^4.54 + t^4.58 + 2*t^4.8 + t^5.06 + 3*t^5.28 + t^5.52 + 5*t^5.76 + t^5.98 - 4*t^6. + t^6.02 + t^6.2 + 3*t^6.24 + t^6.28 - t^6.48 + 2*t^6.74 + 3*t^6.96 + t^6.98 + 4*t^7.18 + 2*t^7.2 + t^7.22 + t^7.24 + 3*t^7.42 + t^7.44 + t^7.46 + 3*t^7.64 + t^7.66 + t^7.68 + t^7.7 + t^7.72 + 5*t^7.92 + t^7.94 + t^8.16 + t^8.18 + 2*t^8.2 + 7*t^8.4 + t^8.42 - 4*t^8.64 - t^8.66 + t^8.68 + 2*t^8.86 + 2*t^8.9 - t^4.44/y - (2*t^7.08)/y + t^7.32/y - t^7.56/y + (2*t^7.8)/y + t^8.28/y + (2*t^8.52)/y + (2*t^8.74)/y + (4*t^8.76)/y + (2*t^8.78)/y + t^8.98/y - t^4.44*y - 2*t^7.08*y + t^7.32*y - t^7.56*y + 2*t^7.8*y + t^8.28*y + 2*t^8.52*y + 2*t^8.74*y + 4*t^8.76*y + 2*t^8.78*y + t^8.98*y | (2*t^2.64)/(g1^6*g2^6) + t^2.88/(g1^2*g2^2) + g1^12*t^3.1 + 2*g1^2*g2^2*t^3.12 + (g2^4*t^3.14)/g1^8 + t^4.1/(g1^17*g2^5) + (2*t^4.32)/(g1^3*g2^3) + (3*g1^11*t^4.54)/g2 + (g2^3*t^4.58)/g1^9 + 2*g1^5*g2^5*t^4.8 + (g2^11*t^5.06)/g1 + (3*t^5.28)/(g1^12*g2^12) + t^5.52/(g1^8*g2^8) + (5*t^5.76)/(g1^4*g2^4) + (g1^10*t^5.98)/g2^2 - 4*t^6. + (g2^2*t^6.02)/g1^10 + g1^24*t^6.2 + 3*g1^4*g2^4*t^6.24 + (g2^8*t^6.28)/g1^16 - g1^8*g2^8*t^6.48 + (2*t^6.74)/(g1^23*g2^11) + (3*t^6.96)/(g1^9*g2^9) + t^6.98/(g1^19*g2^7) + (4*g1^5*t^7.18)/g2^7 + (2*t^7.2)/(g1^5*g2^5) + t^7.22/(g1^15*g2^3) + t^7.24/(g1^25*g2) + (3*g1^9*t^7.42)/g2^3 + t^7.44/(g1*g2) + (g2*t^7.46)/g1^11 + (3*g1^23*t^7.64)/g2 + g1^13*g2*t^7.66 + g1^3*g2^3*t^7.68 + (g2^5*t^7.7)/g1^7 + (g2^7*t^7.72)/g1^17 + (4*t^7.92)/(g1^18*g2^18) + g1^7*g2^7*t^7.92 + (g2^9*t^7.94)/g1^3 + t^8.16/(g1^14*g2^14) + g1*g2^13*t^8.18 + t^8.2/(g1^34*g2^10) + (g2^15*t^8.2)/g1^9 + (7*t^8.4)/(g1^10*g2^10) + t^8.42/(g1^20*g2^8) - (4*t^8.64)/(g1^6*g2^6) - t^8.66/(g1^16*g2^4) + t^8.68/(g1^26*g2^2) + (2*g1^8*t^8.86)/g2^4 + (2*t^8.9)/g1^12 - t^4.44/(g1*g2*y) - (2*t^7.08)/(g1^7*g2^7*y) + t^7.32/(g1^3*g2^3*y) - (g1*g2*t^7.56)/y + (2*g1^5*g2^5*t^7.8)/y + t^8.28/(g1^12*g2^12*y) + (2*t^8.52)/(g1^8*g2^8*y) + (2*g1^6*t^8.74)/(g2^6*y) + (4*t^8.76)/(g1^4*g2^4*y) + (2*t^8.78)/(g1^14*g2^2*y) + (g1^10*t^8.98)/(g2^2*y) - (t^4.44*y)/(g1*g2) - (2*t^7.08*y)/(g1^7*g2^7) + (t^7.32*y)/(g1^3*g2^3) - g1*g2*t^7.56*y + 2*g1^5*g2^5*t^7.8*y + (t^8.28*y)/(g1^12*g2^12) + (2*t^8.52*y)/(g1^8*g2^8) + (2*g1^6*t^8.74*y)/g2^6 + (4*t^8.76*y)/(g1^4*g2^4) + (2*t^8.78*y)/(g1^14*g2^2) + (g1^10*t^8.98*y)/g2^2 |
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 |
|---|---|---|---|---|---|---|---|---|
| 55303 | $M_1q_1q_2$ + $ 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_1M_5$ + $ M_2\phi_1^2$ + $ M_6\phi_1^2$ + $ M_5q_2\tilde{q}_1$ | 0.705 | 0.865 | 0.815 | [X:[], M:[1.0399, 1.0399, 0.8803, 0.8803, 0.9601, 1.0399], q:[0.4402, 0.5199], qb:[0.5199, 0.5997], phi:[0.4801]] | 2*t^2.64 + t^2.88 + 4*t^3.12 + t^4.08 + 2*t^4.32 + 4*t^4.56 + 2*t^4.8 + t^5.04 + 3*t^5.28 + t^5.52 + 5*t^5.76 - 2*t^6. - t^4.44/y - t^4.44*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 |
|---|---|---|---|---|---|---|---|---|---|
| 46595 | 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_1M_5$ + $ M_2\phi_1^2$ | 0.709 | 0.8723 | 0.8128 | [X:[], M:[1.0454, 1.0454, 0.8639, 0.8639, 0.9546], q:[0.4363, 0.5184], qb:[0.5184, 0.6177], phi:[0.4773]] | 2*t^2.59 + 2*t^2.86 + t^3.11 + t^3.14 + t^3.16 + t^4.05 + 2*t^4.3 + 3*t^4.54 + t^4.59 + 2*t^4.84 + t^5.14 + 3*t^5.18 + 3*t^5.46 + 5*t^5.73 + 2*t^5.97 - 4*t^6. - t^4.43/y - t^4.43*y | detail |