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 |
|---|---|---|---|---|---|---|---|---|---|
| 56191 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }\phi_{1}^{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{2}q_{2}\tilde{q}_{1}$ + ${ }M_{3}q_{2}\tilde{q}_{2}$ + ${ }M_{2}M_{3}$ + ${ }\phi_{1}\tilde{q}_{2}^{2}$ + ${ }M_{2}M_{4}$ + ${ }M_{5}\phi_{1}q_{2}\tilde{q}_{1}$ + ${ }M_{6}q_{1}\tilde{q}_{1}$ + ${ }M_{7}\phi_{1}\tilde{q}_{1}^{2}$ | 0.6825 | 0.8676 | 0.7867 | [M:[0.8313, 1.2078, 0.7922, 0.7922, 0.7922, 0.8705, 0.8313], q:[0.753, 0.4157], qb:[0.3765, 0.7922], phi:[0.4157]] | [M:[[-4], [-1], [1], [1], [1], [-9], [-4]], q:[[6], [-2]], qb:[[3], [1]], phi:[[-2]]] | 1 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| ${}M_{3}$, ${ }M_{4}$, ${ }M_{5}$, ${ }M_{1}$, ${ }M_{7}$, ${ }\phi_{1}^{2}$, ${ }M_{6}$, ${ }\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}^{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }q_{1}\tilde{q}_{2}$, ${ }M_{3}^{2}$, ${ }M_{3}M_{4}$, ${ }M_{4}^{2}$, ${ }M_{3}M_{5}$, ${ }M_{4}M_{5}$, ${ }M_{5}^{2}$, ${ }\phi_{1}q_{1}q_{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{1}M_{3}$, ${ }M_{1}M_{4}$, ${ }M_{1}M_{5}$, ${ }M_{3}M_{7}$, ${ }M_{4}M_{7}$, ${ }M_{5}M_{7}$, ${ }M_{3}\phi_{1}^{2}$, ${ }M_{4}\phi_{1}^{2}$, ${ }M_{5}\phi_{1}^{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }M_{1}^{2}$, ${ }M_{3}M_{6}$, ${ }M_{4}M_{6}$, ${ }M_{5}M_{6}$, ${ }M_{1}M_{7}$, ${ }M_{7}^{2}$, ${ }M_{1}\phi_{1}^{2}$, ${ }M_{7}\phi_{1}^{2}$, ${ }\phi_{1}^{4}$, ${ }M_{1}M_{6}$, ${ }M_{6}M_{7}$, ${ }M_{6}\phi_{1}^{2}$, ${ }M_{6}^{2}$, ${ }\phi_{1}q_{1}^{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }M_{3}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{4}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{5}\tilde{q}_{1}\tilde{q}_{2}$ | ${}M_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{7}\tilde{q}_{1}\tilde{q}_{2}$ | -1 | 3*t^2.376 + 3*t^2.494 + t^2.612 + t^3.506 + t^3.741 + 2*t^4.635 + 7*t^4.753 + 8*t^4.871 + 8*t^4.988 + 3*t^5.106 + t^5.223 + t^5.765 + 2*t^5.882 - t^6. + 2*t^6.235 + t^6.353 + 3*t^7.012 + 12*t^7.129 + 15*t^7.247 + 18*t^7.365 + 17*t^7.482 + 8*t^7.6 + 3*t^7.717 + t^7.835 + 2*t^8.141 + t^8.259 - 8*t^8.376 - 7*t^8.494 - 5*t^8.612 + 2*t^8.729 + 2*t^8.847 + t^8.964 - t^4.247/y - (2*t^6.624)/y - (3*t^6.741)/y - t^6.859/y + t^7.635/y + (6*t^7.753)/y + (11*t^7.871)/y + (6*t^7.988)/y + (3*t^8.106)/y + (3*t^8.882)/y - t^4.247*y - 2*t^6.624*y - 3*t^6.741*y - t^6.859*y + t^7.635*y + 6*t^7.753*y + 11*t^7.871*y + 6*t^7.988*y + 3*t^8.106*y + 3*t^8.882*y | 3*g1*t^2.376 + (3*t^2.494)/g1^4 + t^2.612/g1^9 + g1^4*t^3.506 + t^3.741/g1^6 + 2*g1^7*t^4.635 + 7*g1^2*t^4.753 + (8*t^4.871)/g1^3 + (8*t^4.988)/g1^8 + (3*t^5.106)/g1^13 + t^5.223/g1^18 + g1^10*t^5.765 + 2*g1^5*t^5.882 - t^6. + (2*t^6.235)/g1^10 + t^6.353/g1^15 + 3*g1^8*t^7.012 + 12*g1^3*t^7.129 + (15*t^7.247)/g1^2 + (18*t^7.365)/g1^7 + (17*t^7.482)/g1^12 + (8*t^7.6)/g1^17 + (3*t^7.717)/g1^22 + t^7.835/g1^27 + 2*g1^11*t^8.141 + g1^6*t^8.259 - 8*g1*t^8.376 - (7*t^8.494)/g1^4 - (5*t^8.612)/g1^9 + (2*t^8.729)/g1^14 + (2*t^8.847)/g1^19 + t^8.964/g1^24 - t^4.247/(g1^2*y) - (2*t^6.624)/(g1*y) - (3*t^6.741)/(g1^6*y) - t^6.859/(g1^11*y) + (g1^7*t^7.635)/y + (6*g1^2*t^7.753)/y + (11*t^7.871)/(g1^3*y) + (6*t^7.988)/(g1^8*y) + (3*t^8.106)/(g1^13*y) + (3*g1^5*t^8.882)/y - (t^4.247*y)/g1^2 - (2*t^6.624*y)/g1 - (3*t^6.741*y)/g1^6 - (t^6.859*y)/g1^11 + g1^7*t^7.635*y + 6*g1^2*t^7.753*y + (11*t^7.871*y)/g1^3 + (6*t^7.988*y)/g1^8 + (3*t^8.106*y)/g1^13 + 3*g1^5*t^8.882*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 |
|---|---|---|---|---|---|---|---|---|---|
| 50974 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }\phi_{1}^{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{2}q_{2}\tilde{q}_{1}$ + ${ }M_{3}q_{2}\tilde{q}_{2}$ + ${ }M_{2}M_{3}$ + ${ }\phi_{1}\tilde{q}_{2}^{2}$ + ${ }M_{2}M_{4}$ + ${ }M_{5}\phi_{1}q_{2}\tilde{q}_{1}$ + ${ }M_{6}q_{1}\tilde{q}_{1}$ | 0.6685 | 0.8428 | 0.7932 | [M:[0.8435, 1.2109, 0.7891, 0.7891, 0.7891, 0.898], q:[0.7347, 0.4218], qb:[0.3673, 0.7891], phi:[0.4218]] | 3*t^2.367 + 2*t^2.531 + t^2.694 + 2*t^3.469 + t^3.796 + 2*t^4.571 + 7*t^4.735 + 5*t^4.898 + 5*t^5.061 + 2*t^5.224 + t^5.388 + t^5.673 + 5*t^5.837 - t^4.265/y - t^4.265*y | detail | {a: 5503/8232, c: 3469/4116, M1: 124/147, M2: 178/147, M3: 116/147, M4: 116/147, M5: 116/147, M6: 44/49, q1: 36/49, q2: 62/147, qb1: 18/49, qb2: 116/147, phi1: 62/147} |