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 |
|---|---|---|---|---|---|---|---|---|---|
| 1934 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{3}q_{1}\tilde{q}_{1}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{1}M_{3}$ + ${ }M_{3}M_{5}$ + ${ }\phi_{1}^{2}q_{2}\tilde{q}_{1}$ + ${ }\phi_{1}q_{2}\tilde{q}_{2}$ + ${ }M_{4}X_{1}$ | 0.6342 | 0.7835 | 0.8094 | [X:[1.6111], M:[0.8334, 0.722, 1.1666, 0.3889, 0.8334], q:[0.3889, 0.7777], qb:[0.4446, 0.8334], phi:[0.3889]] | [X:[[1]], M:[[3], [-7], [-3], [-1], [3]], q:[[-1], [-2]], qb:[[4], [3]], phi:[[-1]]] | 1 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| ${}M_{2}$, ${ }\phi_{1}^{2}$, ${ }M_{1}$, ${ }M_{5}$, ${ }\phi_{1}q_{1}^{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }q_{2}\tilde{q}_{1}$, ${ }q_{1}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{1}^{2}$, ${ }M_{2}^{2}$, ${ }M_{2}\phi_{1}^{2}$, ${ }M_{1}M_{2}$, ${ }M_{2}M_{5}$, ${ }\phi_{1}^{4}$, ${ }\phi_{1}q_{1}q_{2}$, ${ }M_{1}\phi_{1}^{2}$, ${ }M_{5}\phi_{1}^{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }X_{1}$, ${ }M_{1}^{2}$, ${ }M_{1}M_{5}$, ${ }M_{5}^{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{2}\phi_{1}q_{1}^{2}$, ${ }\phi_{1}^{3}q_{1}^{2}$, ${ }\phi_{1}q_{2}^{2}$ | ${}M_{5}\phi_{1}q_{1}^{2}$, ${ }\phi_{1}^{3}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}^{2}q_{1}\tilde{q}_{2}$ | 1 | t^2.166 + t^2.333 + 2*t^2.5 + t^3.5 + 3*t^3.667 + t^3.834 + t^4.332 + t^4.499 + 3*t^4.666 + 3*t^4.833 + 3*t^5.001 + t^5.666 + 2*t^5.833 + t^6. + 5*t^6.167 + 2*t^6.334 + t^6.498 + t^6.665 + 3*t^6.832 + 3*t^6.999 + 3*t^7.167 + 5*t^7.334 + 5*t^7.501 + t^7.668 + t^7.831 + 2*t^7.999 + t^8.333 - t^8.5 + t^8.663 + 6*t^8.668 + t^8.831 + 3*t^8.835 + 3*t^8.998 - t^4.167/y - t^6.332/y - t^6.5/y - t^6.667/y + t^7.499/y + (3*t^7.666)/y + (3*t^7.833)/y + (2*t^8.001)/y - t^8.498/y + (2*t^8.833)/y - t^4.167*y - t^6.332*y - t^6.5*y - t^6.667*y + t^7.499*y + 3*t^7.666*y + 3*t^7.833*y + 2*t^8.001*y - t^8.498*y + 2*t^8.833*y | t^2.166/g1^7 + t^2.333/g1^2 + 2*g1^3*t^2.5 + t^3.5/g1^3 + 3*g1^2*t^3.667 + g1^7*t^3.834 + t^4.332/g1^14 + t^4.499/g1^9 + (3*t^4.666)/g1^4 + 3*g1*t^4.833 + 3*g1^6*t^5.001 + t^5.666/g1^10 + (2*t^5.833)/g1^5 + t^6. + 5*g1^5*t^6.167 + 2*g1^10*t^6.334 + t^6.498/g1^21 + t^6.665/g1^16 + (3*t^6.832)/g1^11 + (3*t^6.999)/g1^6 + (3*t^7.167)/g1 + 5*g1^4*t^7.334 + 5*g1^9*t^7.501 + g1^14*t^7.668 + t^7.831/g1^17 + (2*t^7.999)/g1^12 + t^8.333/g1^2 - g1^3*t^8.5 + t^8.663/g1^28 + 6*g1^8*t^8.668 + t^8.831/g1^23 + 3*g1^13*t^8.835 + (3*t^8.998)/g1^18 - t^4.167/(g1*y) - t^6.332/(g1^8*y) - t^6.5/(g1^3*y) - (g1^2*t^6.667)/y + t^7.499/(g1^9*y) + (3*t^7.666)/(g1^4*y) + (3*g1*t^7.833)/y + (2*g1^6*t^8.001)/y - t^8.498/(g1^15*y) + (2*t^8.833)/(g1^5*y) - (t^4.167*y)/g1 - (t^6.332*y)/g1^8 - (t^6.5*y)/g1^3 - g1^2*t^6.667*y + (t^7.499*y)/g1^9 + (3*t^7.666*y)/g1^4 + 3*g1*t^7.833*y + 2*g1^6*t^8.001*y - (t^8.498*y)/g1^15 + (2*t^8.833*y)/g1^5 |
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 |
|---|---|---|---|---|---|---|---|---|
| 2970 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{3}q_{1}\tilde{q}_{1}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{1}M_{3}$ + ${ }M_{3}M_{5}$ + ${ }\phi_{1}^{2}q_{2}\tilde{q}_{1}$ + ${ }\phi_{1}q_{2}\tilde{q}_{2}$ + ${ }M_{4}X_{1}$ + ${ }M_{6}\phi_{1}q_{1}^{2}$ | 0.6488 | 0.8093 | 0.8017 | [X:[1.6082], M:[0.8245, 0.7428, 1.1755, 0.3918, 0.8245, 0.8245], q:[0.3918, 0.7837], qb:[0.4327, 0.8245], phi:[0.3918]] | t^2.228 + t^2.351 + 3*t^2.474 + 3*t^3.649 + t^3.772 + t^4.457 + t^4.579 + 4*t^4.702 + 4*t^4.825 + 6*t^4.947 + t^5.877 - t^6. - t^4.175/y - t^4.175*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 |
|---|---|---|---|---|---|---|---|---|---|
| 579 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{3}q_{1}\tilde{q}_{1}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{1}M_{3}$ + ${ }M_{3}M_{5}$ + ${ }\phi_{1}^{2}q_{2}\tilde{q}_{1}$ | 0.7283 | 0.8957 | 0.8131 | [M:[0.9749, 0.82, 1.0251, 0.7699, 0.9749], q:[0.4487, 0.5763], qb:[0.5262, 0.6538], phi:[0.4487]] | t^2.31 + t^2.46 + t^2.692 + 2*t^2.925 + 2*t^3.308 + t^4.039 + t^4.271 + t^4.421 + t^4.503 + t^4.62 + 2*t^4.654 + t^4.77 + t^4.804 + t^4.886 + t^4.92 + t^5.002 + t^5.036 + t^5.153 + 2*t^5.235 + t^5.269 + 2*t^5.385 + 2*t^5.617 + 2*t^5.85 - 2*t^6. - t^4.346/y - t^4.346*y | detail |