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 |
|---|---|---|---|---|---|---|---|---|---|
| 295 | SU2adj1nf2 | ${}\phi_{1}q_{1}q_{2}$ + ${ }M_{1}q_{1}\tilde{q}_{1}$ + ${ }M_{2}\phi_{1}\tilde{q}_{2}^{2}$ + ${ }M_{1}M_{2}$ + ${ }M_{1}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{3}\phi_{1}\tilde{q}_{1}^{2}$ | 0.5069 | 0.6453 | 0.7855 | [M:[1.1786, 0.8214, 0.75], q:[0.3929, 1.2143], qb:[0.4286, 0.3929], phi:[0.3929]] | [M:[[3], [-3], [7]], q:[[1], [-2]], qb:[[-4], [1]], phi:[[1]]] | 1 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| ${}M_{3}$, ${ }\phi_{1}^{2}$, ${ }q_{1}\tilde{q}_{2}$, ${ }M_{2}$, ${ }\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{1}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{3}^{2}$, ${ }M_{3}\phi_{1}^{2}$, ${ }M_{3}q_{1}\tilde{q}_{2}$, ${ }M_{2}M_{3}$, ${ }\phi_{1}^{4}$, ${ }M_{3}\tilde{q}_{1}\tilde{q}_{2}$, ${ }q_{1}^{2}\tilde{q}_{2}^{2}$, ${ }M_{2}\phi_{1}^{2}$, ${ }q_{1}q_{2}$, ${ }M_{2}q_{1}\tilde{q}_{2}$, ${ }q_{2}\tilde{q}_{2}$, ${ }\phi_{1}^{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }q_{1}\tilde{q}_{1}\tilde{q}_{2}^{2}$, ${ }M_{2}^{2}$, ${ }q_{2}\tilde{q}_{1}$, ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\tilde{q}_{1}^{2}\tilde{q}_{2}^{2}$, ${ }M_{1}M_{3}$, ${ }M_{1}\phi_{1}^{2}$, ${ }M_{3}\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$ | ${}\phi_{1}^{3}\tilde{q}_{1}\tilde{q}_{2}$ | -1 | t^2.25 + 2*t^2.357 + 2*t^2.464 + t^3.536 + t^3.643 + t^4.5 + 2*t^4.607 + 4*t^4.714 + 5*t^4.821 + 4*t^4.929 + t^5.786 + t^5.893 - t^6. + t^6.75 + 2*t^6.857 + 4*t^6.964 + 7*t^7.071 + 6*t^7.179 + 5*t^7.286 + 5*t^7.393 + t^8.035 + t^8.143 - 2*t^8.25 - 4*t^8.357 - 7*t^8.464 - 2*t^8.572 - t^4.179/y - t^6.428/y - t^6.536/y + (2*t^7.607)/y + (3*t^7.714)/y + (5*t^7.821)/y + (2*t^7.929)/y - t^8.678/y + (2*t^8.893)/y - t^4.179*y - t^6.428*y - t^6.536*y + 2*t^7.607*y + 3*t^7.714*y + 5*t^7.821*y + 2*t^7.929*y - t^8.678*y + 2*t^8.893*y | g1^7*t^2.25 + 2*g1^2*t^2.357 + (2*t^2.464)/g1^3 + g1^3*t^3.536 + t^3.643/g1^2 + g1^14*t^4.5 + 2*g1^9*t^4.607 + 4*g1^4*t^4.714 + (5*t^4.821)/g1 + (4*t^4.929)/g1^6 + g1^10*t^5.786 + g1^5*t^5.893 - t^6. + g1^21*t^6.75 + 2*g1^16*t^6.857 + 4*g1^11*t^6.964 + 7*g1^6*t^7.071 + 6*g1*t^7.179 + (5*t^7.286)/g1^4 + (5*t^7.393)/g1^9 + g1^17*t^8.035 + g1^12*t^8.143 - 2*g1^7*t^8.25 - 4*g1^2*t^8.357 - (7*t^8.464)/g1^3 - (2*t^8.572)/g1^8 - (g1*t^4.179)/y - (g1^8*t^6.428)/y - (g1^3*t^6.536)/y + (2*g1^9*t^7.607)/y + (3*g1^4*t^7.714)/y + (5*t^7.821)/(g1*y) + (2*t^7.929)/(g1^6*y) - (g1^15*t^8.678)/y + (2*g1^5*t^8.893)/y - g1*t^4.179*y - g1^8*t^6.428*y - g1^3*t^6.536*y + 2*g1^9*t^7.607*y + 3*g1^4*t^7.714*y + (5*t^7.821*y)/g1 + (2*t^7.929*y)/g1^6 - g1^15*t^8.678*y + 2*g1^5*t^8.893*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 |
|---|---|---|---|---|---|---|---|---|
| 467 | ${}\phi_{1}q_{1}q_{2}$ + ${ }M_{1}q_{1}\tilde{q}_{1}$ + ${ }M_{2}\phi_{1}\tilde{q}_{2}^{2}$ + ${ }M_{1}M_{2}$ + ${ }M_{1}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{3}\phi_{1}\tilde{q}_{1}^{2}$ + ${ }M_{3}^{2}$ | 0.4739 | 0.6079 | 0.7797 | [M:[1.2857, 0.7143, 1.0], q:[0.4286, 1.1429], qb:[0.2857, 0.4286], phi:[0.4286]] | 2*t^2.143 + 2*t^2.571 + t^3. + t^3.429 + t^3.857 + 4*t^4.286 + 5*t^4.714 + 4*t^5.143 + 2*t^5.571 - t^4.286/y - t^4.286*y | detail | {a: 2601/5488, c: 417/686, M1: 9/7, M2: 5/7, M3: 1, q1: 3/7, q2: 8/7, qb1: 2/7, qb2: 3/7, phi1: 3/7} |
| 468 | ${}\phi_{1}q_{1}q_{2}$ + ${ }M_{1}q_{1}\tilde{q}_{1}$ + ${ }M_{2}\phi_{1}\tilde{q}_{2}^{2}$ + ${ }M_{1}M_{2}$ + ${ }M_{1}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{3}\phi_{1}\tilde{q}_{1}^{2}$ + ${ }M_{4}\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$ | 0.5243 | 0.6766 | 0.775 | [M:[1.1728, 0.8272, 0.7366, 0.7819], q:[0.3909, 1.2181], qb:[0.4362, 0.3909], phi:[0.3909]] | t^2.21 + 3*t^2.346 + 2*t^2.482 + t^3.518 + t^4.42 + 3*t^4.555 + 7*t^4.691 + 7*t^4.827 + 4*t^4.963 + t^5.728 + t^5.864 - 3*t^6. - t^4.173/y - t^4.173*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 |
|---|---|---|---|---|---|---|---|---|---|
| 186 | SU2adj1nf2 | ${}\phi_{1}q_{1}q_{2}$ + ${ }M_{1}q_{1}\tilde{q}_{1}$ + ${ }M_{2}\phi_{1}\tilde{q}_{2}^{2}$ + ${ }M_{1}M_{2}$ + ${ }M_{1}\tilde{q}_{1}\tilde{q}_{2}$ | 0.489 | 0.6143 | 0.7961 | [M:[1.2024, 0.7976], q:[0.4008, 1.1984], qb:[0.3967, 0.4008], phi:[0.4008]] | 2*t^2.393 + 2*t^2.405 + t^3.583 + t^3.595 + t^3.607 + 4*t^4.785 + 5*t^4.798 + 2*t^4.81 + 2*t^5.976 + 2*t^5.988 - t^6. - t^4.202/y - t^4.202*y | detail |