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 |
|---|---|---|---|---|---|---|---|---|---|
| 6446 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{3}q_{1}\tilde{q}_{1}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{5}q_{2}\tilde{q}_{1}$ + ${ }M_{4}M_{5}$ + ${ }\phi_{1}\tilde{q}_{2}^{2}$ + ${ }M_{1}M_{3}$ + ${ }M_{6}\phi_{1}q_{2}^{2}$ + ${ }M_{3}M_{7}$ + ${ }M_{8}\phi_{1}\tilde{q}_{1}^{2}$ + ${ }M_{5}M_{8}$ | 0.6882 | 0.8739 | 0.7875 | [M:[0.9714, 0.8571, 1.0286, 0.8, 1.2, 0.6857, 0.9714, 0.8], q:[0.6, 0.4286], qb:[0.3714, 0.7714], phi:[0.4571]] | [M:[[0], [0], [0], [0], [0], [0], [0], [0]], q:[[0], [0]], qb:[[0], [0]], phi:[[0]]] | 0 | {a: 843/1225, c: 2141/2450, M1: 34/35, M2: 6/7, M3: 36/35, M4: 4/5, M5: 6/5, M6: 24/35, M7: 34/35, M8: 4/5, q1: 3/5, q2: 3/7, qb1: 13/35, qb2: 27/35, phi1: 16/35} |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| ${}M_{6}$, ${ }M_{4}$, ${ }M_{8}$, ${ }M_{2}$, ${ }\phi_{1}^{2}$, ${ }M_{1}$, ${ }M_{7}$, ${ }M_{5}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }M_{6}^{2}$, ${ }q_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }M_{4}M_{6}$, ${ }M_{6}M_{8}$, ${ }\phi_{1}q_{1}q_{2}$, ${ }M_{2}M_{6}$, ${ }M_{4}^{2}$, ${ }M_{4}M_{8}$, ${ }M_{8}^{2}$, ${ }M_{6}\phi_{1}^{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{2}M_{4}$, ${ }M_{1}M_{6}$, ${ }M_{6}M_{7}$, ${ }M_{2}M_{8}$, ${ }\phi_{1}q_{1}^{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }M_{2}^{2}$, ${ }M_{4}\phi_{1}^{2}$, ${ }M_{8}\phi_{1}^{2}$, ${ }M_{1}M_{4}$, ${ }M_{4}M_{7}$, ${ }M_{1}M_{8}$, ${ }M_{7}M_{8}$, ${ }M_{2}\phi_{1}^{2}$, ${ }M_{1}M_{2}$, ${ }M_{2}M_{7}$, ${ }\phi_{1}^{4}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }M_{5}M_{6}$, ${ }M_{1}\phi_{1}^{2}$, ${ }M_{7}\phi_{1}^{2}$, ${ }M_{1}^{2}$, ${ }M_{1}M_{7}$, ${ }M_{7}^{2}$, ${ }M_{6}\phi_{1}q_{2}\tilde{q}_{1}$ | ${}$ | -1 | t^2.057 + 2*t^2.4 + t^2.571 + t^2.743 + 2*t^2.914 + t^3.6 + t^3.771 + 2*t^4.114 + t^4.286 + 3*t^4.457 + t^4.629 + 4*t^4.8 + 5*t^4.971 + 3*t^5.143 + 4*t^5.314 + 2*t^5.486 + 3*t^5.657 + 3*t^5.829 - t^6. + 3*t^6.171 + 2*t^6.343 + 5*t^6.514 + 3*t^6.686 + 4*t^6.857 + 7*t^7.029 + 7*t^7.2 + 8*t^7.371 + 6*t^7.543 + 10*t^7.714 + 8*t^7.886 + 2*t^8.057 + 6*t^8.229 + 2*t^8.4 + 6*t^8.571 + 3*t^8.743 + t^8.914 - t^4.371/y - t^6.429/y - t^6.771/y - t^6.943/y - t^7.114/y - t^7.286/y + (3*t^7.457)/y + (2*t^7.629)/y + (3*t^7.8)/y + (5*t^7.971)/y + (2*t^8.143)/y + (6*t^8.314)/y + t^8.486/y + (3*t^8.657)/y + t^8.829/y - t^4.371*y - t^6.429*y - t^6.771*y - t^6.943*y - t^7.114*y - t^7.286*y + 3*t^7.457*y + 2*t^7.629*y + 3*t^7.8*y + 5*t^7.971*y + 2*t^8.143*y + 6*t^8.314*y + t^8.486*y + 3*t^8.657*y + t^8.829*y | t^2.057 + 2*t^2.4 + t^2.571 + t^2.743 + 2*t^2.914 + t^3.6 + t^3.771 + 2*t^4.114 + t^4.286 + 3*t^4.457 + t^4.629 + 4*t^4.8 + 5*t^4.971 + 3*t^5.143 + 4*t^5.314 + 2*t^5.486 + 3*t^5.657 + 3*t^5.829 - t^6. + 3*t^6.171 + 2*t^6.343 + 5*t^6.514 + 3*t^6.686 + 4*t^6.857 + 7*t^7.029 + 7*t^7.2 + 8*t^7.371 + 6*t^7.543 + 10*t^7.714 + 8*t^7.886 + 2*t^8.057 + 6*t^8.229 + 2*t^8.4 + 6*t^8.571 + 3*t^8.743 + t^8.914 - t^4.371/y - t^6.429/y - t^6.771/y - t^6.943/y - t^7.114/y - t^7.286/y + (3*t^7.457)/y + (2*t^7.629)/y + (3*t^7.8)/y + (5*t^7.971)/y + (2*t^8.143)/y + (6*t^8.314)/y + t^8.486/y + (3*t^8.657)/y + t^8.829/y - t^4.371*y - t^6.429*y - t^6.771*y - t^6.943*y - t^7.114*y - t^7.286*y + 3*t^7.457*y + 2*t^7.629*y + 3*t^7.8*y + 5*t^7.971*y + 2*t^8.143*y + 6*t^8.314*y + t^8.486*y + 3*t^8.657*y + t^8.829*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 |
|---|---|---|---|---|---|---|---|---|---|
| 4831 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{3}q_{1}\tilde{q}_{1}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{5}q_{2}\tilde{q}_{1}$ + ${ }M_{4}M_{5}$ + ${ }\phi_{1}\tilde{q}_{2}^{2}$ + ${ }M_{1}M_{3}$ + ${ }M_{6}\phi_{1}q_{2}^{2}$ + ${ }M_{3}M_{7}$ + ${ }M_{8}\phi_{1}\tilde{q}_{1}^{2}$ | 0.7001 | 0.889 | 0.7875 | [M:[1.0224, 0.7877, 0.9776, 0.8324, 1.1676, 0.7598, 1.0224, 0.6703], q:[0.5838, 0.3938], qb:[0.4386, 0.7737], phi:[0.4525]] | t^2.011 + t^2.279 + t^2.363 + t^2.497 + t^2.715 + 2*t^3.067 + t^3.503 + t^3.855 + t^4.022 + t^4.073 + 2*t^4.29 + t^4.374 + t^4.425 + t^4.508 + t^4.559 + t^4.642 + 2*t^4.726 + t^4.777 + 2*t^4.86 + 2*t^4.995 + 3*t^5.078 + t^5.212 + 2*t^5.347 + 2*t^5.43 + t^5.514 + t^5.564 + 3*t^5.782 + t^5.866 - 2*t^6. - t^4.358/y - t^4.358*y | detail |