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 |
|---|---|---|---|---|---|---|---|---|---|
| 56433 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }M_{3}q_{2}\tilde{q}_{1}$ + ${ }\phi_{1}\tilde{q}_{2}^{2}$ + ${ }M_{3}\phi_{1}^{2}$ + ${ }M_{4}\phi_{1}\tilde{q}_{1}^{2}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{5}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{6}q_{2}\tilde{q}_{2}$ + ${ }M_{1}M_{7}$ | 0.6973 | 0.8712 | 0.8004 | [M:[0.9668, 1.0426, 1.109, 0.7394, 0.8152, 0.7394, 1.0332], q:[0.5498, 0.4834], qb:[0.4076, 0.7773], phi:[0.4455]] | [M:[[-22], [-32], [12], [8], [-2], [8], [22]], q:[[33], [-11]], qb:[[-1], [3]], phi:[[-6]]] | 1 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| ${}M_{4}$, ${ }M_{6}$, ${ }M_{5}$, ${ }\phi_{1}^{2}$, ${ }M_{7}$, ${ }M_{2}$, ${ }M_{3}$, ${ }q_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}q_{2}^{2}$, ${ }M_{4}^{2}$, ${ }M_{4}M_{6}$, ${ }M_{6}^{2}$, ${ }\phi_{1}q_{1}q_{2}$, ${ }\phi_{1}q_{1}^{2}$, ${ }M_{4}M_{5}$, ${ }M_{5}M_{6}$, ${ }M_{5}^{2}$, ${ }M_{4}\phi_{1}^{2}$, ${ }M_{6}\phi_{1}^{2}$, ${ }M_{5}\phi_{1}^{2}$, ${ }M_{4}M_{7}$, ${ }M_{6}M_{7}$, ${ }M_{2}M_{4}$, ${ }M_{2}M_{6}$, ${ }\phi_{1}^{4}$, ${ }M_{3}M_{4}$, ${ }M_{3}M_{6}$, ${ }M_{5}M_{7}$, ${ }M_{3}M_{5}$, ${ }M_{7}\phi_{1}^{2}$ | ${}$ | -2 | 2*t^2.218 + t^2.445 + t^2.673 + t^3.1 + t^3.128 + t^3.327 + t^3.981 + t^4.009 + t^4.209 + t^4.237 + 4*t^4.436 + t^4.636 + 2*t^4.664 + 3*t^4.891 + t^5.118 + 2*t^5.318 + 3*t^5.346 + 3*t^5.545 + t^5.773 - 2*t^6. + 2*t^6.199 + t^6.227 + t^6.255 + 3*t^6.427 + 3*t^6.455 + 7*t^6.654 + t^6.682 + 2*t^6.854 + 3*t^6.882 + 2*t^7.081 + 4*t^7.109 + 2*t^7.308 + 3*t^7.336 + t^7.364 + 3*t^7.536 + 5*t^7.564 + t^7.735 + 4*t^7.763 + t^7.963 + 2*t^7.991 + t^8.019 - 4*t^8.218 + 3*t^8.417 - t^8.445 + 3*t^8.474 + t^8.617 + 5*t^8.645 + 2*t^8.673 + t^8.701 + t^8.844 + 11*t^8.872 - t^4.336/y - (2*t^6.555)/y - t^6.782/y + t^7.209/y + t^7.436/y - t^7.464/y + (2*t^7.664)/y + (3*t^7.891)/y + (3*t^8.118)/y + (2*t^8.318)/y + (2*t^8.346)/y + (3*t^8.545)/y + t^8.573/y - t^8.773/y + t^8.801/y - t^4.336*y - 2*t^6.555*y - t^6.782*y + t^7.209*y + t^7.436*y - t^7.464*y + 2*t^7.664*y + 3*t^7.891*y + 3*t^8.118*y + 2*t^8.318*y + 2*t^8.346*y + 3*t^8.545*y + t^8.573*y - t^8.773*y + t^8.801*y | 2*g1^8*t^2.218 + t^2.445/g1^2 + t^2.673/g1^12 + g1^22*t^3.1 + t^3.128/g1^32 + g1^12*t^3.327 + g1^36*t^3.981 + t^4.009/g1^18 + g1^26*t^4.209 + t^4.237/g1^28 + 4*g1^16*t^4.436 + g1^60*t^4.636 + 2*g1^6*t^4.664 + (3*t^4.891)/g1^4 + t^5.118/g1^14 + 2*g1^30*t^5.318 + (3*t^5.346)/g1^24 + 3*g1^20*t^5.545 + g1^10*t^5.773 - 2*t^6. + 2*g1^44*t^6.199 + t^6.227/g1^10 + t^6.255/g1^64 + 3*g1^34*t^6.427 + (3*t^6.455)/g1^20 + 7*g1^24*t^6.654 + t^6.682/g1^30 + 2*g1^68*t^6.854 + 3*g1^14*t^6.882 + 2*g1^58*t^7.081 + 4*g1^4*t^7.109 + 2*g1^48*t^7.308 + (3*t^7.336)/g1^6 + t^7.364/g1^60 + 3*g1^38*t^7.536 + (5*t^7.564)/g1^16 + g1^82*t^7.735 + 4*g1^28*t^7.763 + g1^72*t^7.963 + 2*g1^18*t^7.991 + t^8.019/g1^36 - 4*g1^8*t^8.218 + 3*g1^52*t^8.417 - t^8.445/g1^2 + (3*t^8.474)/g1^56 + g1^96*t^8.617 + 5*g1^42*t^8.645 + (2*t^8.673)/g1^12 + t^8.701/g1^66 + g1^86*t^8.844 + 11*g1^32*t^8.872 - t^4.336/(g1^6*y) - (2*g1^2*t^6.555)/y - t^6.782/(g1^8*y) + (g1^26*t^7.209)/y + (g1^16*t^7.436)/y - t^7.464/(g1^38*y) + (2*g1^6*t^7.664)/y + (3*t^7.891)/(g1^4*y) + (3*t^8.118)/(g1^14*y) + (2*g1^30*t^8.318)/y + (2*t^8.346)/(g1^24*y) + (3*g1^20*t^8.545)/y + t^8.573/(g1^34*y) - (g1^10*t^8.773)/y + t^8.801/(g1^44*y) - (t^4.336*y)/g1^6 - 2*g1^2*t^6.555*y - (t^6.782*y)/g1^8 + g1^26*t^7.209*y + g1^16*t^7.436*y - (t^7.464*y)/g1^38 + 2*g1^6*t^7.664*y + (3*t^7.891*y)/g1^4 + (3*t^8.118*y)/g1^14 + 2*g1^30*t^8.318*y + (2*t^8.346*y)/g1^24 + 3*g1^20*t^8.545*y + (t^8.573*y)/g1^34 - g1^10*t^8.773*y + (t^8.801*y)/g1^44 |
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 |
|---|---|---|---|---|---|---|---|---|---|
| 52636 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }M_{3}q_{2}\tilde{q}_{1}$ + ${ }\phi_{1}\tilde{q}_{2}^{2}$ + ${ }M_{3}\phi_{1}^{2}$ + ${ }M_{4}\phi_{1}\tilde{q}_{1}^{2}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{5}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{6}q_{2}\tilde{q}_{2}$ | 0.7015 | 0.8773 | 0.7996 | [M:[0.9436, 1.0088, 1.1217, 0.7478, 0.8131, 0.7478], q:[0.5847, 0.4718], qb:[0.4065, 0.7804], phi:[0.4392]] | 2*t^2.243 + t^2.439 + t^2.635 + t^2.831 + t^3.026 + t^3.365 + t^3.952 + t^4.095 + t^4.148 + t^4.291 + 4*t^4.487 + 2*t^4.683 + t^4.825 + 3*t^4.878 + 3*t^5.074 + 4*t^5.27 + t^5.466 + 2*t^5.608 + t^5.661 + t^5.857 - 2*t^6. - t^4.317/y - t^4.317*y | detail |