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 |
|---|---|---|---|---|---|---|---|---|---|
| 4307 | SU2adj1nf2 | ${}\phi_{1}q_{1}q_{2}$ + ${ }M_{1}q_{1}\tilde{q}_{1}$ + ${ }M_{2}\phi_{1}\tilde{q}_{2}^{2}$ + ${ }M_{3}q_{2}\tilde{q}_{1}$ + ${ }M_{4}\phi_{1}\tilde{q}_{1}^{2}$ + ${ }M_{2}M_{5}$ + ${ }M_{1}M_{5}$ + ${ }M_{3}M_{4}$ + ${ }M_{3}M_{6}$ + ${ }M_{5}M_{7}$ + ${ }M_{8}\phi_{1}^{2}$ | 0.5929 | 0.7511 | 0.7894 | [M:[0.6888, 0.6888, 1.0622, 0.9378, 1.3112, 0.9378, 0.6888, 1.1867], q:[0.9834, 0.6099], qb:[0.3278, 0.4523], phi:[0.4066]] | [M:[[-20], [-20], [4], [-4], [20], [-4], [-20], [12]], q:[[15], [-9]], qb:[[5], [13]], phi:[[-6]]] | 1 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| ${}M_{1}$, ${ }M_{7}$, ${ }\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{4}$, ${ }M_{6}$, ${ }q_{2}\tilde{q}_{2}$, ${ }M_{8}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{1}^{2}$, ${ }M_{1}M_{7}$, ${ }M_{7}^{2}$, ${ }q_{1}\tilde{q}_{2}$, ${ }M_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{7}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\tilde{q}_{1}^{2}\tilde{q}_{2}^{2}$, ${ }q_{1}q_{2}$, ${ }M_{1}M_{4}$, ${ }M_{1}M_{6}$, ${ }M_{4}M_{7}$, ${ }M_{6}M_{7}$, ${ }M_{4}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{6}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{1}q_{2}\tilde{q}_{2}$, ${ }M_{7}q_{2}\tilde{q}_{2}$, ${ }q_{2}\tilde{q}_{1}\tilde{q}_{2}^{2}$, ${ }M_{4}^{2}$, ${ }M_{4}M_{6}$, ${ }M_{6}^{2}$, ${ }M_{1}M_{8}$, ${ }M_{7}M_{8}$, ${ }M_{1}\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{7}\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{8}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{1}^{2}\tilde{q}_{2}^{2}$ | ${}M_{4}q_{2}\tilde{q}_{2}$, ${ }M_{6}q_{2}\tilde{q}_{2}$ | -1 | 2*t^2.066 + t^2.34 + 2*t^2.813 + t^3.187 + 2*t^3.56 + 3*t^4.133 + t^4.307 + 2*t^4.407 + t^4.681 + t^4.78 + 4*t^4.88 + 2*t^5.154 + t^5.253 + t^5.527 + 5*t^5.627 + 2*t^5.901 - t^6. + 4*t^6.199 + 4*t^6.373 + 2*t^6.473 + t^6.648 + t^6.747 + 6*t^6.946 + t^7.021 + 3*t^7.12 + 2*t^7.22 + t^7.319 + t^7.494 + 8*t^7.693 + 2*t^7.867 + 3*t^7.967 - 4*t^8.066 + 2*t^8.241 + 5*t^8.265 - t^8.34 + 7*t^8.44 + 2*t^8.539 + t^8.614 + 2*t^8.714 - 5*t^8.813 + t^8.988 - t^4.22/y - (2*t^6.286)/y - t^7.033/y + t^7.133/y + (3*t^7.407)/y + (4*t^7.88)/y + (4*t^8.154)/y + (2*t^8.253)/y - (3*t^8.352)/y + t^8.527/y + (5*t^8.627)/y + (2*t^8.901)/y - t^4.22*y - 2*t^6.286*y - t^7.033*y + t^7.133*y + 3*t^7.407*y + 4*t^7.88*y + 4*t^8.154*y + 2*t^8.253*y - 3*t^8.352*y + t^8.527*y + 5*t^8.627*y + 2*t^8.901*y | (2*t^2.066)/g1^20 + g1^18*t^2.34 + (2*t^2.813)/g1^4 + g1^4*t^3.187 + 2*g1^12*t^3.56 + (3*t^4.133)/g1^40 + g1^28*t^4.307 + (2*t^4.407)/g1^2 + g1^36*t^4.681 + g1^6*t^4.78 + (4*t^4.88)/g1^24 + 2*g1^14*t^5.154 + t^5.253/g1^16 + g1^22*t^5.527 + (5*t^5.627)/g1^8 + 2*g1^30*t^5.901 - t^6. + (4*t^6.199)/g1^60 + 4*g1^8*t^6.373 + (2*t^6.473)/g1^22 + g1^46*t^6.648 + g1^16*t^6.747 + (6*t^6.946)/g1^44 + g1^54*t^7.021 + 3*g1^24*t^7.12 + (2*t^7.22)/g1^6 + t^7.319/g1^36 + g1^32*t^7.494 + (8*t^7.693)/g1^28 + 2*g1^40*t^7.867 + 3*g1^10*t^7.967 - (4*t^8.066)/g1^20 + 2*g1^48*t^8.241 + (5*t^8.265)/g1^80 - g1^18*t^8.34 + (7*t^8.44)/g1^12 + (2*t^8.539)/g1^42 + g1^56*t^8.614 + 2*g1^26*t^8.714 - (5*t^8.813)/g1^4 + g1^64*t^8.988 - t^4.22/(g1^6*y) - (2*t^6.286)/(g1^26*y) - t^7.033/(g1^10*y) + t^7.133/(g1^40*y) + (3*t^7.407)/(g1^2*y) + (4*t^7.88)/(g1^24*y) + (4*g1^14*t^8.154)/y + (2*t^8.253)/(g1^16*y) - (3*t^8.352)/(g1^46*y) + (g1^22*t^8.527)/y + (5*t^8.627)/(g1^8*y) + (2*g1^30*t^8.901)/y - (t^4.22*y)/g1^6 - (2*t^6.286*y)/g1^26 - (t^7.033*y)/g1^10 + (t^7.133*y)/g1^40 + (3*t^7.407*y)/g1^2 + (4*t^7.88*y)/g1^24 + 4*g1^14*t^8.154*y + (2*t^8.253*y)/g1^16 - (3*t^8.352*y)/g1^46 + g1^22*t^8.527*y + (5*t^8.627*y)/g1^8 + 2*g1^30*t^8.901*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 |
|---|---|---|---|---|---|---|---|---|---|
| 2296 | SU2adj1nf2 | ${}\phi_{1}q_{1}q_{2}$ + ${ }M_{1}q_{1}\tilde{q}_{1}$ + ${ }M_{2}\phi_{1}\tilde{q}_{2}^{2}$ + ${ }M_{3}q_{2}\tilde{q}_{1}$ + ${ }M_{4}\phi_{1}\tilde{q}_{1}^{2}$ + ${ }M_{2}M_{5}$ + ${ }M_{1}M_{5}$ + ${ }M_{3}M_{4}$ + ${ }M_{3}M_{6}$ + ${ }M_{5}M_{7}$ | 0.6089 | 0.7794 | 0.7812 | [M:[0.6737, 0.6737, 1.0653, 0.9347, 1.3263, 0.9347, 0.6737], q:[0.9948, 0.6031], qb:[0.3316, 0.4621], phi:[0.4021]] | 2*t^2.021 + t^2.381 + t^2.413 + 2*t^2.804 + t^3.196 + t^3.587 + 3*t^4.042 + t^4.371 + 2*t^4.402 + 2*t^4.434 + t^4.762 + 2*t^4.794 + 5*t^4.825 + 2*t^5.185 + 3*t^5.217 + t^5.577 + 4*t^5.608 + t^5.969 - t^4.206/y - t^4.206*y | detail |