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 |
|---|---|---|---|---|---|---|---|---|---|
| 1181 | SU2adj1nf2 | $\phi_1q_1^2$ + $ M_1q_2\tilde{q}_1$ + $ M_2q_2\tilde{q}_2$ + $ M_3\tilde{q}_1\tilde{q}_2$ + $ M_2\phi_1^2$ + $ M_4\phi_1q_2^2$ + $ M_4q_1\tilde{q}_2$ + $ M_5q_1\tilde{q}_2$ + $ M_6\phi_1q_2\tilde{q}_2$ | 0.7066 | 0.8907 | 0.7932 | [X:[], M:[1.0132, 1.1201, 0.9466, 0.7467, 0.7467, 0.6801], q:[0.78, 0.4067], qb:[0.5802, 0.4733], phi:[0.44]] | [X:[], M:[[32], [-12], [22], [-8], [-8], [-18]], q:[[-3], [1]], qb:[[-33], [11]], phi:[[6]]] | 1 | {a: 302420677/428009496, c: 95310743/107002374, M1: 12836/12669, M2: 4730/4223, M3: 11992/12669, M4: 9460/12669, M5: 9460/12669, M6: 2872/4223, q1: 3294/4223, q2: 5152/12669, qb1: 2450/4223, qb2: 5996/12669, phi1: 1858/4223} |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| $M_6$, $ M_4$, $ M_5$, $ \phi_1^2$, $ M_3$, $ M_1$, $ M_2$, $ q_1q_2$, $ M_6^2$, $ q_1\tilde{q}_1$, $ \phi_1\tilde{q}_2^2$, $ M_4M_6$, $ M_5M_6$, $ \phi_1q_2\tilde{q}_1$, $ M_4^2$, $ M_4M_5$, $ M_5^2$, $ \phi_1\tilde{q}_1\tilde{q}_2$, $ M_6\phi_1^2$, $ \phi_1\tilde{q}_1^2$, $ M_3M_6$, $ M_4\phi_1^2$, $ M_5\phi_1^2$, $ M_3M_4$, $ M_3M_5$, $ M_1M_6$, $ M_1M_4$, $ M_1M_5$, $ \phi_1^4$, $ M_2M_6$, $ M_2M_4$, $ M_2M_5$, $ M_6q_1q_2$, $ M_3^2$, $ M_1\phi_1^2$, $ M_4q_1q_2$, $ M_5q_1q_2$, $ M_1M_3$ | . | -2 | t^2.04 + 2*t^2.24 + t^2.64 + t^2.84 + t^3.04 + t^3.36 + t^3.56 + 2*t^4.08 + t^4.16 + 3*t^4.28 + 4*t^4.48 + t^4.68 + t^4.8 + 3*t^4.88 + 3*t^5.08 + 3*t^5.28 + t^5.4 + 3*t^5.6 + t^5.68 + t^5.8 + t^5.88 - 2*t^6. + t^6.08 + 2*t^6.12 + t^6.2 + 4*t^6.32 + 3*t^6.4 + 5*t^6.52 + 7*t^6.72 + t^6.84 + 4*t^6.92 + 2*t^7.04 + 6*t^7.12 + t^7.2 + 5*t^7.32 + 2*t^7.44 + 4*t^7.52 + 4*t^7.64 + t^7.72 + 4*t^7.84 + 3*t^7.92 - 2*t^8.04 + 3*t^8.12 + 3*t^8.16 - 5*t^8.24 + 3*t^8.32 + 5*t^8.36 + t^8.44 + t^8.52 + 6*t^8.56 + 3*t^8.64 + t^8.72 + 7*t^8.76 - 4*t^8.84 + 2*t^8.88 + t^8.92 + 12*t^8.96 - t^4.32/y - t^6.36/y - (2*t^6.56)/y - t^7.16/y + (3*t^7.28)/y - t^7.36/y + (2*t^7.48)/y + t^7.68/y + (3*t^7.88)/y + (5*t^8.08)/y + (3*t^8.28)/y + t^8.48/y + t^8.6/y + t^8.68/y - t^8.8/y + t^8.88/y - t^4.32*y - t^6.36*y - 2*t^6.56*y - t^7.16*y + 3*t^7.28*y - t^7.36*y + 2*t^7.48*y + t^7.68*y + 3*t^7.88*y + 5*t^8.08*y + 3*t^8.28*y + t^8.48*y + t^8.6*y + t^8.68*y - t^8.8*y + t^8.88*y | t^2.04/g1^18 + (2*t^2.24)/g1^8 + g1^12*t^2.64 + g1^22*t^2.84 + g1^32*t^3.04 + t^3.36/g1^12 + t^3.56/g1^2 + (2*t^4.08)/g1^36 + g1^28*t^4.16 + (3*t^4.28)/g1^26 + (4*t^4.48)/g1^16 + t^4.68/g1^6 + t^4.8/g1^60 + 3*g1^4*t^4.88 + 3*g1^14*t^5.08 + 3*g1^24*t^5.28 + t^5.4/g1^30 + (3*t^5.6)/g1^20 + g1^44*t^5.68 + t^5.8/g1^10 + g1^54*t^5.88 - 2*t^6. + g1^64*t^6.08 + (2*t^6.12)/g1^54 + g1^10*t^6.2 + (4*t^6.32)/g1^44 + 3*g1^20*t^6.4 + (5*t^6.52)/g1^34 + (7*t^6.72)/g1^24 + t^6.84/g1^78 + (4*t^6.92)/g1^14 + (2*t^7.04)/g1^68 + (6*t^7.12)/g1^4 + g1^60*t^7.2 + 5*g1^6*t^7.32 + (2*t^7.44)/g1^48 + 4*g1^16*t^7.52 + (4*t^7.64)/g1^38 + g1^26*t^7.72 + (4*t^7.84)/g1^28 + 3*g1^36*t^7.92 - (2*t^8.04)/g1^18 + 3*g1^46*t^8.12 + (3*t^8.16)/g1^72 - (5*t^8.24)/g1^8 + 3*g1^56*t^8.32 + (5*t^8.36)/g1^62 + g1^2*t^8.44 + g1^66*t^8.52 + (6*t^8.56)/g1^52 + 3*g1^12*t^8.64 + g1^76*t^8.72 + (7*t^8.76)/g1^42 - 4*g1^22*t^8.84 + (2*t^8.88)/g1^96 + g1^86*t^8.92 + (12*t^8.96)/g1^32 - (g1^6*t^4.32)/y - t^6.36/(g1^12*y) - (2*t^6.56)/(g1^2*y) - (g1^28*t^7.16)/y + (3*t^7.28)/(g1^26*y) - (g1^38*t^7.36)/y + (2*t^7.48)/(g1^16*y) + t^7.68/(g1^6*y) + (3*g1^4*t^7.88)/y + (5*g1^14*t^8.08)/y + (3*g1^24*t^8.28)/y + (g1^34*t^8.48)/y + t^8.6/(g1^20*y) + (g1^44*t^8.68)/y - t^8.8/(g1^10*y) + (g1^54*t^8.88)/y - g1^6*t^4.32*y - (t^6.36*y)/g1^12 - (2*t^6.56*y)/g1^2 - g1^28*t^7.16*y + (3*t^7.28*y)/g1^26 - g1^38*t^7.36*y + (2*t^7.48*y)/g1^16 + (t^7.68*y)/g1^6 + 3*g1^4*t^7.88*y + 5*g1^14*t^8.08*y + 3*g1^24*t^8.28*y + g1^34*t^8.48*y + (t^8.6*y)/g1^20 + g1^44*t^8.68*y - (t^8.8*y)/g1^10 + g1^54*t^8.88*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 |
|---|---|---|---|---|---|---|---|---|---|
| 718 | SU2adj1nf2 | $\phi_1q_1^2$ + $ M_1q_2\tilde{q}_1$ + $ M_2q_2\tilde{q}_2$ + $ M_3\tilde{q}_1\tilde{q}_2$ + $ M_2\phi_1^2$ + $ M_4\phi_1q_2^2$ + $ M_4q_1\tilde{q}_2$ + $ M_5q_1\tilde{q}_2$ | 0.6858 | 0.8499 | 0.8069 | [X:[], M:[1.011, 1.1209, 0.945, 0.7473, 0.7473], q:[0.7802, 0.4066], qb:[0.5825, 0.4725], phi:[0.4396]] | 2*t^2.24 + t^2.64 + t^2.84 + t^3.03 + t^3.36 + t^3.56 + t^3.96 + t^4.09 + t^4.15 + t^4.29 + 4*t^4.48 + t^4.81 + 2*t^4.88 + 2*t^5.08 + 3*t^5.27 + 2*t^5.6 + t^5.67 + t^5.8 + t^5.87 - 2*t^6. - t^4.32/y - t^4.32*y | detail |