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 |
|---|---|---|---|---|---|---|---|---|---|
| 822 | SU2adj1nf2 | $M_1q_1q_2$ + $ \phi_1^2\tilde{q}_1\tilde{q}_2$ + $ M_2q_1\tilde{q}_1$ + $ M_3q_2\tilde{q}_2$ + $ M_4q_2\tilde{q}_1$ + $ M_5q_1\tilde{q}_2$ + $ M_1M_3$ + $ M_3M_6$ | 0.7284 | 0.9028 | 0.8068 | [X:[], M:[0.9169, 0.7506, 1.0831, 0.9169, 0.9169, 0.9169], q:[0.6247, 0.4584], qb:[0.6247, 0.4584], phi:[0.4584]] | [X:[], M:[[-2, -2], [-6, -6], [2, 2], [0, 4], [-4, -8], [-2, -2]], q:[[4, 6], [-2, -4]], qb:[[2, 0], [0, 2]], phi:[[-1, -1]]] | 2 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| $M_2$, $ M_5$, $ M_1$, $ M_6$, $ \phi_1^2$, $ M_4$, $ \tilde{q}_1\tilde{q}_2$, $ \phi_1q_2^2$, $ \phi_1q_2\tilde{q}_2$, $ \phi_1\tilde{q}_2^2$, $ M_2^2$, $ \phi_1q_2\tilde{q}_1$, $ \phi_1q_1q_2$, $ \phi_1\tilde{q}_1\tilde{q}_2$, $ \phi_1q_1\tilde{q}_2$, $ M_2M_5$, $ M_1M_2$, $ M_2M_6$, $ M_2\phi_1^2$, $ M_2M_4$, $ \phi_1\tilde{q}_1^2$, $ \phi_1q_1\tilde{q}_1$, $ \phi_1q_1^2$, $ M_5^2$, $ M_1M_5$, $ M_5M_6$, $ M_5\phi_1^2$, $ M_1^2$, $ M_4M_5$, $ M_1M_6$, $ M_6^2$, $ M_1\phi_1^2$, $ M_6\phi_1^2$, $ \phi_1^4$, $ M_2\tilde{q}_1\tilde{q}_2$, $ M_1M_4$, $ M_4M_6$, $ M_4\phi_1^2$, $ M_4^2$ | $M_1\tilde{q}_1\tilde{q}_2$, $ M_4\tilde{q}_1\tilde{q}_2$, $ M_5\tilde{q}_1\tilde{q}_2$, $ M_6\tilde{q}_1\tilde{q}_2$ | -3 | t^2.25 + 5*t^2.75 + t^3.25 + 3*t^4.13 + t^4.5 + 4*t^4.62 + 5*t^5. + 3*t^5.12 + 12*t^5.5 - 3*t^6. + 3*t^6.38 - 4*t^6.5 + t^6.76 + 15*t^6.88 + 5*t^7.25 + 12*t^7.38 + 12*t^7.75 + 4*t^7.87 + 20*t^8.25 - 4*t^8.37 + 3*t^8.63 - 18*t^8.75 - t^4.38/y - t^6.63/y - (4*t^7.13)/y + (4*t^7.62)/y + (5*t^8.)/y + t^8.12/y + (11*t^8.5)/y - t^8.88/y - t^4.38*y - t^6.63*y - 4*t^7.13*y + 4*t^7.62*y + 5*t^8.*y + t^8.12*y + 11*t^8.5*y - t^8.88*y | t^2.25/(g1^6*g2^6) + t^2.75/(g1^4*g2^8) + (3*t^2.75)/(g1^2*g2^2) + g2^4*t^2.75 + g1^2*g2^2*t^3.25 + t^4.13/(g1^5*g2^9) + t^4.13/(g1^3*g2^3) + (g2^3*t^4.13)/g1 + t^4.5/(g1^12*g2^12) + t^4.62/(g1*g2^5) + 2*g1*g2*t^4.62 + g1^3*g2^7*t^4.62 + t^5./(g1^10*g2^14) + (3*t^5.)/(g1^8*g2^8) + t^5./(g1^6*g2^2) + (g1^3*t^5.12)/g2 + g1^5*g2^5*t^5.12 + g1^7*g2^11*t^5.12 + t^5.5/(g1^8*g2^16) + (2*t^5.5)/(g1^6*g2^10) + (6*t^5.5)/(g1^4*g2^4) + (2*g2^2*t^5.5)/g1^2 + g2^8*t^5.5 - t^6. - t^6./(g1^2*g2^6) - g1^2*g2^6*t^6. + t^6.38/(g1^11*g2^15) + t^6.38/(g1^9*g2^9) + t^6.38/(g1^7*g2^3) - (g1^2*t^6.5)/g2^2 - 2*g1^4*g2^4*t^6.5 - g1^6*g2^10*t^6.5 + t^6.76/(g1^18*g2^18) + t^6.88/(g1^9*g2^17) + (4*t^6.88)/(g1^7*g2^11) + (5*t^6.88)/(g1^5*g2^5) + (4*g2*t^6.88)/g1^3 + (g2^7*t^6.88)/g1 + t^7.25/(g1^16*g2^20) + (3*t^7.25)/(g1^14*g2^14) + t^7.25/(g1^12*g2^8) + t^7.38/(g1^5*g2^13) + (3*t^7.38)/(g1^3*g2^7) + (4*t^7.38)/(g1*g2) + 3*g1*g2^5*t^7.38 + g1^3*g2^11*t^7.38 + t^7.75/(g1^14*g2^22) + (2*t^7.75)/(g1^12*g2^16) + (6*t^7.75)/(g1^10*g2^10) + (2*t^7.75)/(g1^8*g2^4) + (g2^2*t^7.75)/g1^6 + t^7.87/(g1*g2^9) + (g1*t^7.87)/g2^3 + g1^5*g2^9*t^7.87 + g1^7*g2^15*t^7.87 + (3*t^8.25)/g1^4 + t^8.25/(g1^12*g2^24) + (3*t^8.25)/(g1^10*g2^18) + (3*t^8.25)/(g1^8*g2^12) + (6*t^8.25)/(g1^6*g2^6) + (3*g2^6*t^8.25)/g1^2 + g2^12*t^8.25 - g1^5*g2*t^8.37 - 2*g1^7*g2^7*t^8.37 - g1^9*g2^13*t^8.37 + t^8.63/(g1^17*g2^21) + t^8.63/(g1^15*g2^15) + t^8.63/(g1^13*g2^9) - (5*t^8.75)/(g1^4*g2^8) - (8*t^8.75)/(g1^2*g2^2) - 5*g2^4*t^8.75 - t^4.38/(g1*g2*y) - t^6.63/(g1^7*g2^7*y) - t^7.13/(g1^5*g2^9*y) - (2*t^7.13)/(g1^3*g2^3*y) - (g2^3*t^7.13)/(g1*y) + t^7.62/(g1*g2^5*y) + (2*g1*g2*t^7.62)/y + (g1^3*g2^7*t^7.62)/y + t^8./(g1^10*g2^14*y) + (3*t^8.)/(g1^8*g2^8*y) + t^8./(g1^6*g2^2*y) + (g1^5*g2^5*t^8.12)/y + (3*t^8.5)/(g1^6*g2^10*y) + (5*t^8.5)/(g1^4*g2^4*y) + (3*g2^2*t^8.5)/(g1^2*y) - t^8.88/(g1^13*g2^13*y) - (t^4.38*y)/(g1*g2) - (t^6.63*y)/(g1^7*g2^7) - (t^7.13*y)/(g1^5*g2^9) - (2*t^7.13*y)/(g1^3*g2^3) - (g2^3*t^7.13*y)/g1 + (t^7.62*y)/(g1*g2^5) + 2*g1*g2*t^7.62*y + g1^3*g2^7*t^7.62*y + (t^8.*y)/(g1^10*g2^14) + (3*t^8.*y)/(g1^8*g2^8) + (t^8.*y)/(g1^6*g2^2) + g1^5*g2^5*t^8.12*y + (3*t^8.5*y)/(g1^6*g2^10) + (5*t^8.5*y)/(g1^4*g2^4) + (3*g2^2*t^8.5*y)/g1^2 - (t^8.88*y)/(g1^13*g2^13) |
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 |
|---|---|---|---|---|---|---|---|---|---|
| 526 | SU2adj1nf2 | $M_1q_1q_2$ + $ \phi_1^2\tilde{q}_1\tilde{q}_2$ + $ M_2q_1\tilde{q}_1$ + $ M_3q_2\tilde{q}_2$ + $ M_4q_2\tilde{q}_1$ + $ M_5q_1\tilde{q}_2$ + $ M_1M_3$ | 0.7211 | 0.8891 | 0.811 | [X:[], M:[0.9247, 0.774, 1.0753, 0.9247, 0.9247], q:[0.613, 0.4623], qb:[0.613, 0.4623], phi:[0.4623]] | t^2.32 + 4*t^2.77 + 2*t^3.23 + 3*t^4.16 + 4*t^4.61 + t^4.64 + 3*t^5.07 + 4*t^5.1 + 8*t^5.55 - t^4.39/y - t^4.39*y | detail |