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 |
|---|---|---|---|---|---|---|---|---|---|
| 56142 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }M_{3}q_{2}\tilde{q}_{1}$ + ${ }\phi_{1}\tilde{q}_{2}^{2}$ + ${ }M_{3}\phi_{1}^{2}$ + ${ }M_{4}\phi_{1}q_{2}\tilde{q}_{1}$ + ${ }M_{3}M_{5}$ + ${ }M_{6}\phi_{1}q_{2}^{2}$ + ${ }\phi_{1}q_{1}^{2}$ + ${ }M_{7}q_{2}\tilde{q}_{2}$ | 0.682 | 0.8746 | 0.7798 | [M:[0.7728, 0.8272, 1.2, 0.8, 0.8, 0.7456, 0.7728], q:[0.8, 0.4272], qb:[0.3728, 0.8], phi:[0.4]] | [M:[[1], [-1], [0], [0], [0], [2], [1]], q:[[0], [-1]], qb:[[1], [0]], phi:[[0]]] | 1 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| ${}M_{6}$, ${ }M_{1}$, ${ }M_{7}$, ${ }M_{4}$, ${ }M_{5}$, ${ }\phi_{1}^{2}$, ${ }M_{2}$, ${ }\phi_{1}\tilde{q}_{1}^{2}$, ${ }\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{6}^{2}$, ${ }M_{1}M_{6}$, ${ }M_{6}M_{7}$, ${ }M_{1}^{2}$, ${ }M_{4}M_{6}$, ${ }M_{5}M_{6}$, ${ }M_{1}M_{7}$, ${ }M_{7}^{2}$, ${ }M_{6}\phi_{1}^{2}$, ${ }M_{1}M_{4}$, ${ }M_{1}M_{5}$, ${ }M_{2}M_{6}$, ${ }M_{4}M_{7}$, ${ }M_{5}M_{7}$, ${ }M_{1}\phi_{1}^{2}$, ${ }M_{7}\phi_{1}^{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }M_{1}M_{2}$, ${ }M_{4}^{2}$, ${ }M_{4}M_{5}$, ${ }M_{5}^{2}$, ${ }M_{2}M_{7}$, ${ }M_{4}\phi_{1}^{2}$, ${ }M_{5}\phi_{1}^{2}$, ${ }\phi_{1}^{4}$, ${ }q_{1}\tilde{q}_{2}$, ${ }M_{2}M_{4}$, ${ }M_{2}M_{5}$, ${ }M_{2}\phi_{1}^{2}$, ${ }\phi_{1}q_{1}q_{2}$, ${ }M_{2}^{2}$, ${ }M_{6}\phi_{1}\tilde{q}_{1}^{2}$, ${ }M_{1}\phi_{1}\tilde{q}_{1}^{2}$, ${ }M_{7}\phi_{1}\tilde{q}_{1}^{2}$, ${ }M_{6}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{4}\phi_{1}\tilde{q}_{1}^{2}$, ${ }M_{5}\phi_{1}\tilde{q}_{1}^{2}$, ${ }\phi_{1}^{3}\tilde{q}_{1}^{2}$, ${ }M_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{7}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{2}\phi_{1}\tilde{q}_{1}^{2}$, ${ }M_{4}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{5}\tilde{q}_{1}\tilde{q}_{2}$ | ${}M_{2}\tilde{q}_{1}\tilde{q}_{2}$ | -2 | t^2.237 + 2*t^2.318 + 3*t^2.4 + t^2.482 + t^3.437 + t^3.518 + t^4.474 + 2*t^4.555 + 6*t^4.637 + 7*t^4.718 + 9*t^4.8 + 3*t^4.882 + t^4.963 + t^5.674 + 3*t^5.755 + 4*t^5.837 + 2*t^5.918 - 2*t^6. - 2*t^6.082 - t^6.163 + t^6.711 + 2*t^6.792 + 7*t^6.874 + 12*t^6.955 + 17*t^7.037 + 16*t^7.118 + 15*t^7.2 + 5*t^7.282 + t^7.363 + t^7.445 + t^7.911 + 3*t^7.992 + 7*t^8.074 + 9*t^8.155 + 5*t^8.237 - 5*t^8.318 - 13*t^8.4 - 12*t^8.482 - 6*t^8.563 - t^8.645 + t^8.947 - t^4.2/y - t^6.437/y - (2*t^6.518)/y - (2*t^6.6)/y - t^6.682/y + (2*t^7.555)/y + (4*t^7.637)/y + (8*t^7.718)/y + (7*t^7.8)/y + (5*t^7.882)/y + t^7.963/y + t^8.755/y - t^8.918/y - t^4.2*y - t^6.437*y - 2*t^6.518*y - 2*t^6.6*y - t^6.682*y + 2*t^7.555*y + 4*t^7.637*y + 8*t^7.718*y + 7*t^7.8*y + 5*t^7.882*y + t^7.963*y + t^8.755*y - t^8.918*y | g1^2*t^2.237 + 2*g1*t^2.318 + 3*t^2.4 + t^2.482/g1 + g1^2*t^3.437 + g1*t^3.518 + g1^4*t^4.474 + 2*g1^3*t^4.555 + 6*g1^2*t^4.637 + 7*g1*t^4.718 + 9*t^4.8 + (3*t^4.882)/g1 + t^4.963/g1^2 + g1^4*t^5.674 + 3*g1^3*t^5.755 + 4*g1^2*t^5.837 + 2*g1*t^5.918 - 2*t^6. - (2*t^6.082)/g1 - t^6.163/g1^2 + g1^6*t^6.711 + 2*g1^5*t^6.792 + 7*g1^4*t^6.874 + 12*g1^3*t^6.955 + 17*g1^2*t^7.037 + 16*g1*t^7.118 + 15*t^7.2 + (5*t^7.282)/g1 + t^7.363/g1^2 + t^7.445/g1^3 + g1^6*t^7.911 + 3*g1^5*t^7.992 + 7*g1^4*t^8.074 + 9*g1^3*t^8.155 + 5*g1^2*t^8.237 - 5*g1*t^8.318 - 13*t^8.4 - (12*t^8.482)/g1 - (6*t^8.563)/g1^2 - t^8.645/g1^3 + g1^8*t^8.947 - t^4.2/y - (g1^2*t^6.437)/y - (2*g1*t^6.518)/y - (2*t^6.6)/y - t^6.682/(g1*y) + (2*g1^3*t^7.555)/y + (4*g1^2*t^7.637)/y + (8*g1*t^7.718)/y + (7*t^7.8)/y + (5*t^7.882)/(g1*y) + t^7.963/(g1^2*y) + (g1^3*t^8.755)/y - (g1*t^8.918)/y - t^4.2*y - g1^2*t^6.437*y - 2*g1*t^6.518*y - 2*t^6.6*y - (t^6.682*y)/g1 + 2*g1^3*t^7.555*y + 4*g1^2*t^7.637*y + 8*g1*t^7.718*y + 7*t^7.8*y + (5*t^7.882*y)/g1 + (t^7.963*y)/g1^2 + g1^3*t^8.755*y - g1*t^8.918*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 |
|---|---|---|---|---|---|---|---|---|---|
| 50875 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }M_{3}q_{2}\tilde{q}_{1}$ + ${ }\phi_{1}\tilde{q}_{2}^{2}$ + ${ }M_{3}\phi_{1}^{2}$ + ${ }M_{4}\phi_{1}q_{2}\tilde{q}_{1}$ + ${ }M_{3}M_{5}$ + ${ }M_{6}\phi_{1}q_{2}^{2}$ + ${ }\phi_{1}q_{1}^{2}$ | 0.6642 | 0.8416 | 0.7892 | [M:[0.7807, 0.8193, 1.2, 0.8, 0.8, 0.7613], q:[0.8, 0.4193], qb:[0.3807, 0.8], phi:[0.4]] | t^2.284 + t^2.342 + 3*t^2.4 + t^2.458 + t^3.484 + t^3.542 + t^3.658 + t^4.568 + t^4.626 + 4*t^4.684 + 4*t^4.742 + 8*t^4.8 + 3*t^4.858 + t^4.916 + t^5.768 + 2*t^5.826 + 3*t^5.884 + 3*t^5.942 - t^6. - t^4.2/y - t^4.2*y | detail |