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 |
|---|---|---|---|---|---|---|---|---|---|
| 3401 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{3}q_{1}\tilde{q}_{1}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{5}q_{2}\tilde{q}_{1}$ + ${ }M_{4}M_{5}$ + ${ }\phi_{1}q_{1}\tilde{q}_{1}$ + ${ }M_{3}X_{1}$ + ${ }M_{2}\phi_{1}q_{2}^{2}$ + ${ }M_{4}M_{6}$ | 0.6499 | 0.8094 | 0.803 | [X:[1.6121], M:[0.7456, 0.806, 0.3879, 1.1637, 0.8363, 0.8363], q:[0.8514, 0.403], qb:[0.7607, 0.4332], phi:[0.3879]] | [X:[[4]], M:[[-18], [2], [-4], [-12], [12], [12]], q:[[17], [1]], qb:[[-13], [11]], phi:[[-4]]] | 1 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| ${}M_{1}$, ${ }\phi_{1}^{2}$, ${ }M_{2}$, ${ }M_{5}$, ${ }M_{6}$, ${ }\phi_{1}q_{2}^{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{2}^{2}$, ${ }q_{1}\tilde{q}_{2}$, ${ }M_{1}^{2}$, ${ }M_{1}\phi_{1}^{2}$, ${ }M_{1}M_{2}$, ${ }\phi_{1}^{4}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }M_{1}M_{5}$, ${ }M_{1}M_{6}$, ${ }M_{2}\phi_{1}^{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{2}^{2}$, ${ }M_{5}\phi_{1}^{2}$, ${ }M_{6}\phi_{1}^{2}$, ${ }X_{1}$, ${ }M_{2}M_{5}$, ${ }M_{2}M_{6}$, ${ }\phi_{1}q_{1}q_{2}$, ${ }M_{5}^{2}$, ${ }M_{5}M_{6}$, ${ }M_{6}^{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$ | ${}\phi_{1}^{3}q_{2}\tilde{q}_{2}$, ${ }M_{1}\phi_{1}\tilde{q}_{2}^{2}$ | 0 | t^2.237 + t^2.327 + t^2.418 + 2*t^2.509 + t^3.582 + t^3.673 + t^3.763 + t^3.854 + t^4.474 + t^4.564 + 2*t^4.655 + 3*t^4.746 + 4*t^4.836 + 2*t^4.927 + 3*t^5.018 + 3*t^6.091 + 3*t^6.181 + 3*t^6.272 + 2*t^6.363 + t^6.71 + t^6.801 + 2*t^6.892 + 3*t^6.982 + 3*t^7.073 + 4*t^7.164 + 4*t^7.254 + 5*t^7.345 + 3*t^7.436 + 5*t^7.526 + t^7.617 + t^7.708 - t^8.146 - 2*t^8.237 - 2*t^8.327 - 2*t^8.418 + 5*t^8.599 + 6*t^8.69 + 5*t^8.781 + 3*t^8.871 + t^8.947 - t^4.164/y - t^6.401/y - t^6.491/y - t^6.582/y - t^6.673/y + t^7.564/y + (2*t^7.655)/y + (4*t^7.746)/y + (3*t^7.836)/y + (3*t^7.927)/y + t^8.018/y - t^8.637/y - t^8.728/y - t^8.819/y - t^4.164*y - t^6.401*y - t^6.491*y - t^6.582*y - t^6.673*y + t^7.564*y + 2*t^7.655*y + 4*t^7.746*y + 3*t^7.836*y + 3*t^7.927*y + t^8.018*y - t^8.637*y - t^8.728*y - t^8.819*y | t^2.237/g1^18 + t^2.327/g1^8 + g1^2*t^2.418 + 2*g1^12*t^2.509 + t^3.582/g1^2 + g1^8*t^3.673 + g1^18*t^3.763 + g1^28*t^3.854 + t^4.474/g1^36 + t^4.564/g1^26 + (2*t^4.655)/g1^16 + (3*t^4.746)/g1^6 + 4*g1^4*t^4.836 + 2*g1^14*t^4.927 + 3*g1^24*t^5.018 + 3*g1^10*t^6.091 + 3*g1^20*t^6.181 + 3*g1^30*t^6.272 + 2*g1^40*t^6.363 + t^6.71/g1^54 + t^6.801/g1^44 + (2*t^6.892)/g1^34 + (3*t^6.982)/g1^24 + (3*t^7.073)/g1^14 + (4*t^7.164)/g1^4 + 4*g1^6*t^7.254 + 5*g1^16*t^7.345 + 3*g1^26*t^7.436 + 5*g1^36*t^7.526 + g1^46*t^7.617 + g1^56*t^7.708 - t^8.146/g1^28 - (2*t^8.237)/g1^18 - (2*t^8.327)/g1^8 - 2*g1^2*t^8.418 + 5*g1^22*t^8.599 + 6*g1^32*t^8.69 + 5*g1^42*t^8.781 + 3*g1^52*t^8.871 + t^8.947/g1^72 - t^4.164/(g1^4*y) - t^6.401/(g1^22*y) - t^6.491/(g1^12*y) - t^6.582/(g1^2*y) - (g1^8*t^6.673)/y + t^7.564/(g1^26*y) + (2*t^7.655)/(g1^16*y) + (4*t^7.746)/(g1^6*y) + (3*g1^4*t^7.836)/y + (3*g1^14*t^7.927)/y + (g1^24*t^8.018)/y - t^8.637/(g1^40*y) - t^8.728/(g1^30*y) - t^8.819/(g1^20*y) - (t^4.164*y)/g1^4 - (t^6.401*y)/g1^22 - (t^6.491*y)/g1^12 - (t^6.582*y)/g1^2 - g1^8*t^6.673*y + (t^7.564*y)/g1^26 + (2*t^7.655*y)/g1^16 + (4*t^7.746*y)/g1^6 + 3*g1^4*t^7.836*y + 3*g1^14*t^7.927*y + g1^24*t^8.018*y - (t^8.637*y)/g1^40 - (t^8.728*y)/g1^30 - (t^8.819*y)/g1^20 |
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 |
|---|---|---|---|---|---|---|---|---|---|
| 2844 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{3}q_{1}\tilde{q}_{1}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{5}q_{2}\tilde{q}_{1}$ + ${ }M_{4}M_{5}$ + ${ }\phi_{1}q_{1}\tilde{q}_{1}$ + ${ }M_{3}X_{1}$ + ${ }M_{2}\phi_{1}q_{2}^{2}$ | 0.6363 | 0.7853 | 0.8103 | [X:[1.6169], M:[0.7237, 0.8085, 0.3831, 1.1492, 0.8508], q:[0.872, 0.4042], qb:[0.7449, 0.4466], phi:[0.3831]] | t^2.171 + t^2.298 + t^2.425 + t^2.553 + t^3.447 + t^3.575 + t^3.702 + t^3.829 + t^3.956 + t^4.342 + t^4.47 + 2*t^4.597 + 2*t^4.724 + 3*t^4.851 + t^4.978 + t^5.105 + t^5.619 + t^5.746 + t^5.873 + t^6. - t^4.149/y - t^4.149*y | detail |